Semiconductor device

ABSTRACT

Provided is a semiconductor device which is capable of preventing an increase in power consumption of an SGT, i.e., a three-dimensional semiconductor transistor, due to an increase in off-leak current. The semiconductor device comprises: a first-conductive type first silicon pillar: a first dielectric surrounding a side surface of the first silicon pillar; a gate surrounding the dielectric; a second silicon pillar provided underneath the first silicon pillar; and a third silicon pillar provided on a top of the first silicon pillar. The second silicon pillar has a second-conductive type high-concentration impurity region formed in a surface thereof except at least a part of a contact surface region with the first silicon pillar, and a first-conductive type impurity region formed therein and surrounded by the second-conductive type high-concentration impurity region. The third silicon pillar has a second-conductive type high-concentration impurity region formed in a surface thereof except at least a part of a contact surface region with the first silicon pillar, and a first-conductive type impurity region formed therein and surrounded by the second-conductive type high-concentration impurity region of the third silicon pillar. The first-conductive type impurity region of each of the second silicon pillar and the third silicon pillar has a length greater than that of a depletion layer extending from a base portion of the second-conductive type high-concentration impurity region of a respective one of the second silicon pillar and the third silicon pillar.

RELATED APPLICATIONS

Pursuant to 35 U.S.C. §119(e), this application claims the benefit of the filing date of Provisional U.S. Patent Application Ser. No. 61/217,595 filed on Jun. 2, 2009. This application also claims priority under 35 U.S.C. §119(a) to JP2009-130583 filed on May 29, 2009. The entire contents of these applications are hereby incorporated by reference.

BACKGROUND OF THE INVENTION

1. Field of the Invention

The present invention relates to a semiconductor device, and more specifically to a semiconductor device having a surrounding gate transistor (SGT) which is a three-dimensional semiconductor.

2. Description of the Related Art

Based on miniaturization, a planar transistor is used in a wide range of fields, such as computers, communication devices, measurement devices, automatic control devices and domestic devices, as a low-power consumption, low-cost, high-throughput microprocessor, ASIC or microcomputer, and a low-cost, large-capacity memory. However, the planar transistor is two-dimensionally formed on a semiconductor substrate. Specifically, in the planar transistor, a source, a gate and a drain are horizontally structured on a surface of a silicon substrate. In contrast, an SGT is formed in a structure where a source, a gate and a drain are arranged in a vertical direction with respect to a silicon substrate, wherein the gate is formed to surround a convex semiconductor layer (see, for example, the following Non-Patent Document 1, FIG. 144). Thus, in the SGT, an occupancy area can be largely reduced as compared with the planar transistor.

However, in the SGT, a gate length becomes shorter along with miniaturization of ultra-large-scale integrated (ULSI) circuits, so that an off-leak current, i.e., a drain current when a voltage is applied to a drain electrode under a condition that a voltage applied to each of a gate electrode and a source electrode is zero V, becomes larger.

As means to reduce such an off-leak current, there has been known a technique of forming a source and a drain in a cup-like or concave structure, as disclosed, for example, in the following Non-Patent Document 2 and Patent Document 1.

An SGT structure having a conventional source/drain structure as disclosed in the Non-Patent Document 2 is shown in FIGS. 139 and 140. As is clear, particularly, from FIG. 140, the conventional source/drain structure has a horizontally flat distribution. Differently, in a source formed in a concave structure as shown in FIGS. 141 and 142, a potential barrier between the source and a pillar body during application of a voltage to a drain can be increased as compared with the conventional structure, to provide a higher punch-through voltage. Particularly, a much higher punch-through voltage can be provided by reducing a length X which is a depth of a source or drain.

Further, as disclosed in the Patent Document 1, it is also studied to form each of a source and a drain in a concave structure (FIG. 143).

PRIOR ART DOCUMENT

-   -   [Patent Document 1] JP 2007-123415A     -   [Non-Patent Document 1] H. Takato et al., IEEE Transaction on         Electron Devices, Vol. 38, No. 3, March 1991, pp. 573-578     -   [Non-Patent Document 2] R. Nishi, Journal C of the Institute of         Electronics, Information and Communication Engineers (IEICE),         Vol. J86-C, No. 2, February 2003, pp. 200-201,

SUMMARY OF THE INVENTION

The above conventional SGT structure is designed such that only a source region having a concave structure is sufficiently small, or each of a source region and a drain region has a concave structure. Practically, in a source or drain region having a concave structure, it is desirable that a region surrounded by the concave source or drain region is sufficiently large.

The present invention has been made in view of the above circumstances, and it is an object thereof to provide a semiconductor device designed such that a source and/or a drain are formed in a concave shape to solve a problem that power consumption of an SGT is increased due to an increase in off-leak current.

In order to achieve the above object, according to one aspect of the present invention, there is provided a semiconductor device which comprises: a first-conductive type first silicon pillar: a first dielectric surrounding a side surface of the first silicon pillar; a gate surrounding the dielectric; a second silicon pillar provided underneath the first silicon pillar; and a third silicon pillar provided on a top of the first silicon pillar, wherein: the second silicon pillar has a second-conductive type high-concentration impurity region formed in a surface thereof except at least a part of a contact surface region with the first silicon pillar, and a first-conductive type impurity region formed therein and surrounded by the second-conductive type high-concentration impurity region; and the third silicon pillar has a second-conductive type high-concentration impurity region formed in a surface thereof except at least a part of a contact surface region with the first silicon pillar, and a first-conductive type impurity region formed therein and surrounded by the second-conductive type high-concentration impurity region of the third silicon pillar, and wherein the first-conductive type impurity region of each of the second silicon pillar and the third silicon pillar has a length greater than that of a depletion layer extending from a base portion of a respective one of the second silicon pillar and the third silicon pillar.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 is a bird's-eye view showing a semiconductor device according to a first embodiment of the present invention.

FIG. 2 is a sectional view of the semiconductor device, taken along the cutting-plane line a-a′ in FIG. 1.

FIG. 3 is a sectional view of the semiconductor device, taken along the cutting-plane line b-b′ in FIG. 2.

FIG. 4 is a sectional view of the semiconductor device, taken along the cutting-plane line c-c′ in FIG. 2.

FIG. 5 is a sectional view of the semiconductor device, taken along the cutting-plane line d-d′ in FIG. 2.

FIG. 6 is a diagram showing a depletion layer in a silicon pillar of the semiconductor device illustrated in FIG. 1, wherein the depletion layer is divided into a plurality of elements extending from respective ones of a gate, a base portion and a side portion of a concave source diffusion layer, and a base portion and a side portion of a concave drain diffusion layer.

FIG. 7 is a diagram showing a process for performing ion implantation at an oblique angle to form the concave diffusion layers of the semiconductor device illustrated in FIG. 1.

FIG. 8 is a bird's-eye view showing a semiconductor device according to a second embodiment of the present invention.

FIG. 9 is a sectional view of the semiconductor device, taken along the cutting-plane line a-a′ in FIG. 8.

FIG. 10 is a sectional view of the semiconductor device, taken along the cutting-plane line b-b′ in FIG. 9.

FIG. 11 is a sectional view of the semiconductor device, taken along the cutting-plane line c-c′ in FIG. 9.

FIG. 12 is a sectional view of the semiconductor device, taken along the cutting-plane line d-d′ in FIG. 9.

FIG. 13 is a diagram showing a depletion layer in a silicon pillar of the semiconductor device illustrated in FIG. 8, wherein the depletion layer is divided into a plurality of elements extending from respective ones of a gate, a base portion and a side portion of a concave source diffusion layer, and a drain diffusion layer.

FIG. 14 is a diagram showing a process for performing ion implantation at an oblique angle to form the concave diffusion layer of the semiconductor device illustrated in FIG. 8.

FIG. 15 is a bird's-eye view showing a semiconductor device according to a third embodiment of the present invention.

FIG. 16 is a sectional view of the semiconductor device, taken along the cutting-plane line a-a′ in FIG. 15.

FIG. 17 is a sectional view of the semiconductor device, taken along the cutting-plane line b-b′ in FIG. 16.

FIG. 18 is a sectional view of the semiconductor device, taken along the cutting-plane line c-c′ in FIG. 16.

FIG. 19 is a sectional view of the semiconductor device, taken along the cutting-plane line d-d′ in FIG. 16.

FIG. 20 is a diagram showing a depletion layer in a silicon pillar of the semiconductor device illustrated in FIG. 15, wherein the depletion layer is divided into a plurality of elements extending from respective ones of a gate, a base portion and a side portion of a concave source diffusion layer, and a drain diffusion layer.

FIG. 21 is a diagram showing a process for performing ion implantation at an oblique angle to form the concave diffusion layer of the semiconductor device illustrated in FIG. 15.

FIG. 22 is a graph showing a relationship between a punch-through voltage and a length Ls (Ld) in each of the semiconductor devices illustrated in FIGS. 1, 8 and 15.

FIG. 23 is graph showing a relationship between a length Ls (Ld) and a length Lg in the semiconductor device illustrated in FIG. 1.

FIG. 24 is a graph showing a relationship between a punch-through voltage and a diameter Ts or Td in each of the semiconductor devices illustrated in FIGS. 1, 8 and 15.

FIG. 25 is graph showing a relationship between a diameter Ts (Td) and a length Lg in the semiconductor device illustrated in FIG. 1.

FIG. 26 is a bird's-eye view showing a semiconductor device according to a fourth embodiment of the present invention.

FIG. 27 is a sectional view of the semiconductor device, taken along the cutting-plane line a-a′ in FIG. 26.

FIG. 28 is a sectional view of the semiconductor device, taken along the cutting-plane line b-b′ in FIG. 27.

FIG. 29 is a sectional view of the semiconductor device, taken along the cutting-plane line c-c′ in FIG. 27.

FIG. 30 is a sectional view of the semiconductor device, taken along the cutting-plane line d-d′ in FIG. 27.

FIG. 31 is a bird's-eye view showing a semiconductor device according to a fifth embodiment of the present invention.

FIG. 32 is a sectional view of the semiconductor device, taken along the cutting-plane line a-a′ in FIG. 31.

FIG. 33 is a sectional view of the semiconductor device, taken along the cutting-plane line b-b′ in FIG. 32.

FIG. 34 is a sectional view of the semiconductor device, taken along the cutting-plane line c-c′ in FIG. 32.

FIG. 35 is a sectional view of the semiconductor device, taken along the cutting-plane line d-d′ in FIG. 32.

FIG. 36 is a bird's-eye view showing a semiconductor device according to a sixth embodiment of the present invention.

FIG. 37 is a sectional view of the semiconductor device, taken along the cutting-plane line a-a′ in FIG. 36.

FIG. 38 is a sectional view of the semiconductor device, taken along the cutting-plane line b-b′ in FIG. 37.

FIG. 39 is a sectional view of the semiconductor device, taken along the cutting-plane line c-c′ in FIG. 37.

FIG. 40 is a sectional view of the semiconductor device, taken along the cutting-plane line d-d′ in FIG. 37.

FIG. 41 is a graph showing a relationship between a punch-through voltage and a length Ls (Ld) in each of the semiconductor devices illustrated in FIGS. 26, 31 and 36.

FIG. 42 is a graph showing a relationship between a punch-through voltage and a diameter Ts (Td) in each of the semiconductor devices illustrated in FIGS. 26, 31 and 36.

FIG. 43 is a bird's-eye view showing a semiconductor device according to a seventh embodiment of the present invention.

FIG. 44 is a sectional view of the semiconductor device, taken along the cutting-plane line a-a′ in FIG. 43.

FIG. 45 is a sectional view of the semiconductor device, taken along the cutting-plane line b-b′ in FIG. 44.

FIG. 46 is a sectional view of the semiconductor device, taken along the cutting-plane line c-c′ in FIG. 44.

FIG. 47 is a sectional view of the semiconductor device, taken along the cutting-plane line d-d′ in FIG. 44.

FIG. 48 is a bird's-eye view showing a semiconductor device according to an eighth embodiment of the present invention.

FIG. 49 is a sectional view of the semiconductor device, taken along the cutting-plane line a-a′ in FIG. 48.

FIG. 50 is a sectional view of the semiconductor device, taken along the cutting-plane line b-b′ in FIG. 49.

FIG. 51 is a sectional view of the semiconductor device, taken along the cutting-plane line c-c′ in FIG. 49.

FIG. 52 is a sectional view of the semiconductor device, taken along the cutting-plane line d-d′ in FIG. 49.

FIG. 53 is a bird's-eye view showing a semiconductor device according to a ninth embodiment of the present invention.

FIG. 54 is a sectional view of the semiconductor device, taken along the cutting-plane line a-a′ in FIG. 53.

FIG. 55 is a sectional view of the semiconductor device, taken along the cutting-plane line b-b′ in FIG. 54.

FIG. 56 is a sectional view of the semiconductor device, taken along the cutting-plane line c-c′ in FIG. 54.

FIG. 57 is a sectional view of the semiconductor device, taken along the cutting-plane line d-d′ in FIG. 54.

FIG. 58 is a graph showing a relationship between a punch-through voltage and a diameter Ts (Td) in each of the semiconductor devices illustrated in FIGS. 43, 48 and 53.

FIG. 59 is a bird's-eye view showing a semiconductor device according to a tenth embodiment of the present invention.

FIG. 60 is a sectional view of the semiconductor device, taken along the cutting-plane line a-a′ in FIG. 59.

FIG. 61 is a sectional view of the semiconductor device, taken along the cutting-plane line b-b′ in FIG. 60.

FIG. 62 is a sectional view of the semiconductor device, taken along the cutting-plane line c-c′ in FIG. 60.

FIG. 63 is a sectional view of the semiconductor device, taken along the cutting-plane line d-d′ in FIG. 60.

FIG. 64 is a bird's-eye view showing a semiconductor device according to an eleventh embodiment of the present invention.

FIG. 65 is a sectional view of the semiconductor device, taken along the cutting-plane line a-a′ in FIG. 64.

FIG. 66 is a sectional view of the semiconductor device, taken along the cutting-plane line b-b′ in FIG. 65.

FIG. 67 is a sectional view of the semiconductor device, taken along the cutting-plane line c-c′ in FIG. 65.

FIG. 68 is a sectional view of the semiconductor device, taken along the cutting-plane line d-d′ in FIG. 65.

FIG. 69 is a bird's-eye view showing a semiconductor device according to a twelfth embodiment of the present invention.

FIG. 70 is a sectional view of the semiconductor device, taken along the cutting-plane line a-a′ in FIG. 69.

FIG. 71 is a sectional view of the semiconductor device, taken along the cutting-plane line b-b′ in FIG. 70.

FIG. 72 is a sectional view of the semiconductor device, taken along the cutting-plane line c-c′ in FIG. 70.

FIG. 73 is a sectional view of the semiconductor device, taken along the cutting-plane line d-d′ in FIG. 70.

FIG. 74 is a graph showing a relationship between a punch-through voltage and a diameter Ts (Td) in each of the semiconductor devices illustrated in FIGS. 59, 64 and 69.

FIG. 75 is a bird's-eye view showing a semiconductor device according to a thirteenth embodiment of the present invention.

FIG. 76 is a sectional view of the semiconductor device, taken along the cutting-plane line a-a′ in FIG. 75.

FIG. 77 is a sectional view of the semiconductor device, taken along the cutting-plane line b-b′ in FIG. 76.

FIG. 78 is a sectional view of the semiconductor device, taken along the cutting-plane line c-c′ in FIG. 76.

FIG. 79 is a graph showing a relationship between a punch-through voltage and a length Ls in the semiconductor device illustrated in FIG. 75.

FIG. 80 is a graph showing a relationship between a punch-through voltage and a diameter Ts (Td) in the semiconductor device illustrated in FIG. 75.

FIG. 81 is a diagram showing a process for performing ion implantation at an oblique angle to form a concave diffusion layer of the semiconductor device illustrated in FIG. 75.

FIG. 82 is a bird's-eye view showing a semiconductor device according to a fourteenth embodiment of the present invention.

FIG. 83 is a sectional view of the semiconductor device, taken along the cutting-plane line a-a′ in FIG. 82.

FIG. 84 is a sectional view of the semiconductor device, taken along the cutting-plane line b-b′ in FIG. 83.

FIG. 85 is a sectional view of the semiconductor device, taken along the cutting-plane line c-c′ in FIG. 83.

FIG. 86 is a graph showing a relationship between a punch-through voltage and Ls, Ld in the semiconductor device illustrated in FIG. 82.

FIG. 87 is a graph showing a relationship between a punch-through voltage and a diameter Ts (Td) in the semiconductor device illustrated in FIG. 82.

FIG. 88 is a bird's-eye view showing a semiconductor device according to a fifteenth embodiment of the present invention.

FIG. 89 is a sectional view of the semiconductor device, taken along the cutting-plane line a-a′ in FIG. 88.

FIG. 90 is a sectional view of the semiconductor device, taken along the cutting-plane line b-b′ in FIG. 89.

FIG. 91 is a sectional view of the semiconductor device, taken along the cutting-plane line c-c′ in FIG. 89.

FIG. 92 is a graph showing a relationship between a punch-through voltage and Ls, Ld in the semiconductor device illustrated in FIG. 88.

FIG. 93 is a graph showing a relationship between a punch-through voltage and a diameter Ts (Td) in the semiconductor device illustrated in FIG. 88.

FIG. 94 is a diagram showing a process for performing ion implantation at an oblique angle to form a concave diffusion layer of the semiconductor device illustrated in FIG. 88.

FIG. 95 is a bird's-eye view showing a semiconductor device according to a sixteenth embodiment of the present invention.

FIG. 96 is a sectional view of the semiconductor device, taken along the cutting-plane line a-a′ in FIG. 95.

FIG. 97 is a sectional view of the semiconductor device, taken along the cutting-plane line b-b′ in FIG. 96.

FIG. 98 is a sectional view of the semiconductor device, taken along the cutting-plane line c-c′ in FIG. 96.

FIG. 99 is a graph showing a relationship between a punch-through voltage and Ls, Ld in the semiconductor device illustrated in FIG. 95.

FIG. 100 is a graph showing a relationship between a punch-through voltage and a diameter Ts (Td) in the semiconductor device illustrated in FIG. 95.

FIG. 101 is a bird's-eye view showing a semiconductor device according to a seventeenth embodiment of the present invention.

FIG. 102 is a sectional view of the semiconductor device, taken along the cutting-plane line a-a′ in FIG. 101.

FIG. 103 is a sectional view of the semiconductor device, taken along the cutting-plane line b-b′ in FIG. 102.

FIG. 104 is a sectional view of the semiconductor device, taken along the cutting-plane line c-c′ in FIG. 102.

FIG. 105 is a sectional view of the semiconductor device, taken along the cutting-plane line d-d′ in FIG. 102.

FIG. 106 is a bird's-eye view showing a semiconductor device according to an eighteenth embodiment of the present invention.

FIG. 107 is a sectional view of the semiconductor device, taken along the cutting-plane line a-a′ in FIG. 106.

FIG. 108 is a sectional view of the semiconductor device, taken along the cutting-plane line b-b′ in FIG. 107.

FIG. 109 is a sectional view of the semiconductor device, taken along the cutting-plane line c-c′ in FIG. 107.

FIG. 110 is a sectional view of the semiconductor device, taken along the cutting-plane line d-d′ in FIG. 107.

FIG. 111 is a bird's-eye view showing a semiconductor device according to a nineteenth embodiment of the present invention.

FIG. 112 is a sectional view of the semiconductor device, taken along the cutting-plane line a-a′ in FIG. 111.

FIG. 113 is a sectional view of the semiconductor device, taken along the cutting-plane line b-b′ in FIG. 112.

FIG. 114 is a sectional view of the semiconductor device, taken along the cutting-plane line c-c′ in FIG. 112.

FIG. 115 is a sectional view of the semiconductor device, taken along the cutting-plane line d-d′ in FIG. 112.

FIG. 116 is a bird's-eye view showing a semiconductor device according to a twentieth embodiment of the present invention.

FIG. 117 is a sectional view of the semiconductor device, taken along the cutting-plane line a-a′ in FIG. 116.

FIG. 118 is a sectional view of the semiconductor device, taken along the cutting-plane line b-b′ in FIG. 117.

FIG. 119 is a sectional view of the semiconductor device, taken along the cutting-plane line c-c′ in FIG. 117.

FIG. 120 is a sectional view of the semiconductor device, taken along the cutting-plane line d-d′ in FIG. 117.

FIG. 121 is a bird's-eye view showing a semiconductor device according to a twenty-first embodiment of the present invention.

FIG. 122 is a sectional view of the semiconductor device, taken along the cutting-plane line a-a′ in FIG. 121.

FIG. 123 is a sectional view of the semiconductor device, taken along the cutting-plane line b-b′ in FIG. 122.

FIG. 124 is a sectional view of the semiconductor device, taken along the cutting-plane line c-c′ in FIG. 122.

FIG. 125 is a sectional view of the semiconductor device, taken along the cutting-plane line d-d′ in FIG. 122.

FIG. 126 is a bird's-eye view showing a semiconductor device according to a twenty-second embodiment of the present invention.

FIG. 127 is a sectional view of the semiconductor device, taken along the cutting-plane line a-a′ in FIG. 126.

FIG. 128 is a sectional view of the semiconductor device, taken along the cutting-plane line b-b′ in FIG. 127.

FIG. 129 is a sectional view of the semiconductor device, taken along the cutting-plane line c-c′ in FIG. 127.

FIG. 130 is a sectional view of the semiconductor device, taken along the cutting-plane line d-d′ in FIG. 127.

FIG. 131 is a bird's-eye view showing a semiconductor device according to a twenty-third embodiment of the present invention.

FIG. 132 is a sectional view of the semiconductor device, taken along the cutting-plane line a-a′ in FIG. 131.

FIG. 133 is a sectional view of the semiconductor device, taken along the cutting-plane line b-b′ in FIG. 132.

FIG. 134 is a sectional view of the semiconductor device, taken along the cutting-plane line c-c′ in FIG. 132.

FIG. 135 is a bird's-eye view showing a semiconductor device according to a twenty-fourth embodiment of the present invention.

FIG. 136 is a sectional view of the semiconductor device, taken along the cutting-plane line a-a′ in FIG. 135.

FIG. 137 is a sectional view of the semiconductor device, taken along the cutting-plane line b-b′ in FIG. 136.

FIG. 138 is a sectional view of the semiconductor device, taken along the cutting-plane line c-c′ in FIG. 136.

FIG. 139 is a perspective view showing a structure of one example of a conventional SGT.

FIG. 140 is a sectional view showing the structure of the conventional SGT.

FIG. 141 is a perspective view showing a structure of another example of the conventional SGT.

FIG. 142 is a sectional view showing the structure of the conventional SGT.

FIG. 143 is a perspective view showing a structure of yet another example of the conventional SGT.

FIG. 144 is a perspective view showing a structure of still another example of the conventional SGT.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS

With reference to the drawings, a semiconductor device of the present invention will now be specifically described.

(First Embodiment) Semiconductor Device

FIG. 1 is a bird's-eye view showing a semiconductor device according to a first embodiment of the present invention. FIG. 2 is a schematic sectional view taken along the cutting-plane line a-a′ in FIG. 1. FIG. 3 is a schematic sectional view taken along the cutting-plane line b-b′ in FIG. 2. FIG. 4 is a schematic sectional view taken along the cutting-plane line c-c′ in FIG. 2. FIG. 5 is a schematic sectional view taken along the cutting-plane line d-d′ in FIG. 2.

The semiconductor device according to the first embodiment comprises a first-conductive type third silicon pillar 830, a first dielectric 310 surrounding a side surface of the third silicon pillar 830, a gate 210 surrounding the dielectric 310, a first silicon pillar 810 provided underneath the third silicon pillar 830, and a second silicon pillar 820 provided on a top of the third silicon pillar 830, wherein: the first silicon pillar 810 has a second-conductive type high-concentration impurity region 610 (i.e., concave drain diffusion layer 610) formed in a surface thereof except at least a part of a contact surface region with the third silicon pillar 830, and a first-conductive type impurity region 510 formed therein and surrounded by the second-conductive type high-concentration impurity region 610; and the second silicon pillar 820 has a second-conductive type high-concentration impurity region 710 (i.e., concave source diffusion layer 710) formed in a surface thereof except at least a part of a contact surface region with the third silicon pillar 830, and a first-conductive type impurity region 520 formed therein and surrounded by the second-conductive type high-concentration impurity region 710.

In this configuration, as for the impurity region 510 of the first silicon pillar 810 having a circular columnar shape, an outer peripheral surface except an upper surface thereof is covered by an inner surface of the drain diffusion layer 610 having an angular-U shape in vertical section. Similarly, as for the impurity region 520 of the second silicon pillar 820 having a circular columnar shape, an outer peripheral surface except a lower surface thereof is covered by an inner surface of the source diffusion layer 710 having an inversed angular-U shape in vertical section.

In the first embodiment, in view of providing a higher punch-through voltage, it is desirable that each of the first-conductive type impurity region 510 of the first silicon pillar 810 and the first-conductive type impurity region 520 of the second silicon pillar 820 has a sufficiently-large area. In other words, it is desirable that a diameter Td and a height (height dimension) Ld of the first-conductive type impurity region 510, and a diameter Ts and a height (height dimension) Ls of the first-conductive type impurity region 520, are sufficiently large.

As a specific example, assuming a structure in which: a length of the gate 210 is 100 nm; a film thickness of the gate dielectric is 2 nm; a diameter of the first silicon pillar 810 is 100 nm; a height (height dimension) of each of the second silicon pillar 820 and the third silicon pillar 830 is 100 nm; and the diameter Td of the impurity region 510 and the diameter Ts of the impurity region 520 is fixed to 80 nm, a simulation was performed. As a simulation result on this structure, FIG. 22 shows a structure dependence of the punch-through voltage.

The vertical axis of FIG. 22 represents the punch-through voltage Vpt. As used herein, the term “punch-through voltage” means a voltage which is applied to a drain electrode so as to cause a drain current of 1e-7 A/um under a condition that a voltage applied to each of a gate electrode and a source electrode is zero V. The horizontal axis of FIG. 22 represents the height Ld of the impurity region 510 and the height Ls of the impurity region 520. Thus, FIG. 22 shows how the punch-through voltage is changed when each of the height Ld of the impurity region 510 and the height Ls of the impurity region 520 is changed, i.e., shows a dependence of the punch-through voltage on each of the heights Ld, Ls. In FIG. 22, a polygonal line 2201 indicates the simulation result on the semiconductor device according to the first embodiment, and each of two polygonal lines 2202, 2203 indicates a simulation result on a respective one of two semiconductor devices according to after-mentioned second and third embodiments of the present invention. Further, a point 2200 indicates a simulation result on a conventional SGT (SGT having horizontally flat source and drain diffusion layers) as shown in FIGS. 123 and 124.

The simulation result illustrated in FIG. 22 indicates that, in the semiconductor device according to the first embodiment (polygonal line 2201), a higher punch-through voltage as compared with the conventional SGT (point 2200) is provided at any value of each of the heights Ls, Ld other than zero. In other words, it is proven that the semiconductor device according to the first embodiment has an SGT structure with a smaller off-leak current than that in the conventional SGT.

FIG. 23 is a graph showing a dependence of each of the heights Ld, Ls on the gate length Lg, in the semiconductor device according to the first embodiment. In FIG. 23, a region A expressed by a plurality of vertical lines corresponds to a region where a Sub threshold swing is equal to or less than 90 mV/dec. As used herein, the term “Sub threshold swing” means a gate voltage value at a sub-threshold area which changes a drain current by one decade with a drain voltage held constant.

As is clear from FIG. 23, in the conventional SGT (having a SGT structure with horizontally flat source and drain diffusion layers) where Ls=Ld=zero, it is necessary to set the gate length Lg to 102 nm or more, in order to allow the Sub threshold swing to fall within the region where it is equal to or less than 90 mV/dec. In contrast, in the semiconductor device according to the first embodiment, for example, as long as each of the heights Ls, Ld is equal to or greater than 50 nm, the gate length Lg may be set to 94 nm or more to allow the Sub threshold swing to become equal to or less than 90 mV/dec.

FIG. 24 is a graph showing a dependence of the punch-through voltage on each of the diameters Ts, Td, in the semiconductor device according to the first embodiment, by comparison with the conventional SGT. In FIG. 24, the vertical axis represents the punch-through voltage, and the horizontal axis represents the diameter Td of the impurity region 510 and the diameter Ts of the impurity region 520. In FIG. 24, a polygonal line 2401 indicates the simulation result on the semiconductor device according to the first embodiment, and each of two polygonal lines 2402, 2403 indicates the simulation result on a respective one of the two semiconductor devices according to the after-mentioned second and third embodiments. Further, a point 2400 indicates the simulation result on the conventional SGT (SGT having horizontally flat source and drain diffusion layers) as shown in FIGS. 123 and 124.

As is clear from FIG. 24, in the semiconductor device according to the first embodiment, a higher punch-through voltage is provided at any value of each of the diameters Ts, Td other than zero. In other words, it is proven that the semiconductor device according to the first embodiment (polygonal line 2401) has an SGT structure with a smaller off-leak current than that in the conventional SGT (point 2400).

FIG. 25 shows a dependence of each of the diameters Td, Ts on the gate length Lg, in the semiconductor device according to the first embodiment. In FIG. 25, a region B expressed by a plurality of vertical lines corresponds to the region where the Sub threshold swing is equal to or less than 90 mV/dec.

As is clear from FIG. 25, in the conventional SGT (having a SGT structure with horizontally flat source and drain diffusion layers) where Ts=Td=zero, it is necessary to set the gate length Lg to 107 nm or more, in order to allow the Sub threshold swing to fall within the region where it is equal to or less than 90 mV/dec. In contrast, in the semiconductor device according to the first embodiment, for example, as long as each of the heights Ls, Ld is equal to or greater than 80 nm, the gate length Lg may be set to 94 nm or more to allow the Sub threshold swing to become equal to or less than 90 mV/dec.

The following discussion will be made based on a structure illustrated in FIG. 6 to show a preferred value of each of the diameter Td and the height Ld of the impurity region 510 and the diameter Ts and the height Ls of the impurity region 520. In a complete depletion-type SGT, a depletion layer in the entire silicon pillar is divided into a depletion layer 2270 extending from the gate, a depletion layer 2230 extending from a base portion of the concave source diffusion layer, a depletion layer 2240 extending from a side portion of the concave source diffusion layer, a diffusion layer 2210 extending from a base portion of the concave drain diffusion layer, and a depletion layer 2220 extending from a side portion of the concave drain diffusion layer. When an applied voltage is zero V, a depth of the depletion layer 2230 extending from the base portion of the concave source diffusion layer is Ts/4. Thus, as a prerequisite to suppressing a punch-through effect due to contact between the depletion layer 2230 extending from the base portion of the concave source diffusion layer and each of the depletion layers 2210, 2220 extending from the concave drain diffusion layer, it is essential that the height Ls is greater than the depth “Ts/4” of the depletion layer. In other words, it is essential to satisfy the following relation (1-1):

$\begin{matrix} {{Ls} > \frac{Ts}{4}} & \left( {1\text{-}1} \right) \end{matrix}$

Similarly, a depth of the depletion layer 2220 extending from the base portion of the concave drain diffusion layer is Td/4. Thus, as a prerequisite to suppressing a punch-through effect due to contact between the depletion layer 2210 extending from the base portion of the concave drain diffusion layer and each of the depletion layers 2230, 2240 extending from the concave source diffusion layer, it is essential that the height Ld is greater than the depth “Td/4” of the depletion layer. In other words, it is essential to satisfy the following relation (1-2):

$\begin{matrix} {{Ld} > \frac{Td}{4}} & \left( {1\text{-}2} \right) \end{matrix}$

Further, in a process for making the concave diffusion layer-type SGT structure illustrated in FIG. 2, it is necessary to perform ion implantation at an oblique angle as shown in FIG. 7 so as to form the concave diffusion layers. During the ion implantation, for example, when As⁺ is implanted into an NMOSFET, a silicon pillar of an NMOSFET adjacent to the target NMOSFET is likely to disturb the ion implantation. Thus, it is essential to satisfy the following relation (1-3):

$\begin{matrix} {{\tan\left( \frac{\pi}{36} \right)} > \frac{{Ls} + {Ld} + {Lg} + {Ljs} + {Ljd}}{Tspace}} & \left( {1\text{-}3} \right) \end{matrix}$

wherein: Ld is a height of the first-conductive type impurity region 510;

Ls is a height of the first-conductive type impurity region 520;

Lg is a length of the gate;

Ljd is a depth of the second-conductive type high-concentration impurity region 610;

Ljs is a depth of the second-conductive type high-concentration impurity region 620; and

Tspace is a distance between silicon pillars of adjacent two SGTs.

Thus, based on the relation (1-3), (Ls+Ld) is required to satisfy the following relation (1-4):

$\begin{matrix} {{{{\tan\left( \frac{\pi}{36} \right)} \cdot {Tspace}} - \left( {{Lg} + {Ljs} + {Ljd}} \right)} > {{Ls} + {Ld}}} & \left( {1\text{-}4} \right) \end{matrix}$ (Second Embodiment) Semiconductor Device

FIG. 8 is a schematic bird's-eye view of a transistor as a semiconductor device of the present invention, wherein the first-conductive type impurity region 510 of the first silicon pillar 810 in the first embodiment is also formed as a second-conductive type high-concentration impurity region, in addition to the second-conductive type high-concentration impurity region 610 of the first silicon pillar 810. FIG. 9 is a schematic sectional view taken along the cutting-plane line a-a′ in FIG. 8, and FIG. 10 is a schematic sectional view taken along the cutting-plane line b-b′ in FIG. 9. FIG. 11 is a schematic sectional view taken along the cutting-plane line c-c′ in FIG. 9, and FIG. 12 is a schematic sectional view taken along the cutting-plane line d-d′ in FIG. 9.

In the second embodiment, in view of providing a higher punch-through voltage, it is desirable that a first-conductive type impurity region 520 provided in a second silicon pillar 820 has a sufficiently-large area. In other words, it is desirable that a diameter Ts and a height Ls of the first-conductive type impurity region 520 are sufficiently large.

Specifically, assuming a structure in which: a length of a gate 210 is 100 nm; a film thickness of a gate dielectric is 2 nm; a diameter of a first silicon pillar is 100 nm; and a height of each of the second silicon pillar 820 and a third silicon pillar 830 is 100 nm, a simulation was performed. As a simulation result on this structure, FIG. 22 shows a structure dependence of the punch-through voltage. The vertical axis of FIG. 22 represents the punch-through voltage (Vpt) which is a voltage applied to a drain electrode so as to cause a drain current of 1e-7A/um under a condition that a voltage applied to each of a gate electrode and a source electrode is zero V. The horizontal axis represents the height Ls which varies according to a change in shape of a concave source diffusion layer. As see in FIG. 22, in the concave source diffusion layer-type SGT structure (polygonal line 2202), a higher punch-through voltage as compared with the horizontally flat source/drain diffusion layer-type SGT structure (conventional SGT structure indicated by the point 2200) is provided at any value of the height Ls other than zero, which is proven that the SGT structure has a small off-leak current.

FIG. 24 shows a dependence of the punch-through voltage on Ts, Td which varies according to a change in shape of the concave source diffusion layer. As seen in FIG. 24, in the concave source diffusion layer-type SGT structure (polygonal line 2402), a higher punch-through voltage as compared with the horizontally flat source/drain diffusion layer-type SGT structure (conventional SGT structure indicated by the point 2400) is also provided at any value of the diameter Ts other than zero, which is proven that the SGT structure has a small off-leak current.

Based on a structure illustrated in FIG. 13, the following discussion will be made about the height Ls. In a complete depletion-type SGT, a depletion layer in the entire silicon pillar is divided into four depletion layers extending from respective ones of the gate, a base portion and a side portion of the concave source diffusion layer, and a drain diffusion layer. When an applied voltage is zero V, a depth of the depletion layer 2230 extending from the base portion of the concave source diffusion layer is Ts/4. Thus, as a prerequisite to suppressing a punch-through effect due to contact between the depletion layer 2230 extending from the base portion of the concave source diffusion layer and the depletion layer 2250 extending from the drain diffusion layer, it is essential that the height Ls is greater than the depth “Ts/4” of the depletion layer. In other words, it is essential to satisfy the following relation (2-1):

$\begin{matrix} {{Ls} > \frac{Ts}{4}} & \left( {2\text{-}1} \right) \end{matrix}$

Further, in a process for making the concave diffusion layer-type SGT structure illustrated in FIG. 9, it is necessary to perform ion implantation at an oblique angle as shown in FIG. 14 so as to form the concave diffusion layer. During the ion implantation, for example, when As⁺ is implanted into an NMOSFET, a silicon pillar of an NMOSFET adjacent to the target NMOSFET is likely to disturb the ion implantation. Thus, it is essential to satisfy the following relation (2-2):

$\begin{matrix} {{{\tan\left( \frac{\pi}{36} \right)} > \frac{{Ls} + {Lg} + {Ljs} + {Ljd}}{Tspace}},} & \left( {2\text{-}2} \right) \end{matrix}$

wherein: Ls is a height of the first-conductive type impurity region 510;

Lg is a length of the gate;

Ljd is a depth of the second-conductive type high-concentration impurity region 610;

Ljs is a depth of the second-conductive type high-concentration impurity region 620; and

Tspace is a distance between silicon pillars of adjacent two SGTs;

Thus, based on the relation (2-2), Ls is required to satisfy the following relation (2-3):

$\begin{matrix} {{{{\tan\left( \frac{\pi}{36} \right)} \cdot {Tspace}} - \left( {{Lg} + {Ljs} + {Ljd}} \right)} > {Ls}} & \left( {2\text{-}3} \right) \end{matrix}$ (Third Embodiment) Semiconductor Device

FIG. 15 is a schematic bird's-eye view of a transistor as a semiconductor device of the present invention, wherein the first-conductive type impurity region 520 of the second silicon pillar 820 in the first embodiment is also formed as a second-conductive type high-concentration impurity region, in addition to the second-conductive type high-concentration impurity region 710 of the second silicon pillar 820. FIG. 16 is a schematic sectional view taken along the cutting-plane line a-a′ in FIG. 15, and FIG. 17 is a schematic sectional view taken along the cutting-plane line b-b′ in FIG. 16. FIG. 18 is a schematic sectional view taken along the cutting-plane line c-c′ in FIG. 16, and FIG. 19 is a schematic sectional view taken along the cutting-plane line d-d′ in FIG. 16.

In the third embodiment, in view of providing a higher punch-through voltage, it is desirable that a first-conductive type impurity region 510 provided in a first silicon pillar 810 has a sufficiently-large area. In other words, it is desirable that a diameter Td and a height Ld of the first-conductive type impurity region 510 are sufficiently large.

Specifically, assuming a structure in which: a length of a gate 210 is 100 nm; a film thickness of a gate dielectric 310 is 2 nm; a diameter of the first silicon pillar 810 is 100 nm; and a height of each of a second silicon pillar 820 and a third silicon pillar 830 is 100 nm, a simulation was performed. As a simulation result on this structure, FIG. 22 shows a structure dependence of the punch-through voltage. The vertical axis of FIG. 22 represents the punch-through voltage which is a voltage applied to a drain electrode so as to cause a drain current of 1e-7A/um under a condition that a voltage applied to each of a gate electrode and a source electrode is zero V. The horizontal axis represents the height Ld which varies according to a change in shape of a concave drain diffusion layer. As seen in FIG. 22, in the concave drain diffusion layer-type SGT structure, a higher punch-through voltage as compared with the horizontally flat source/drain diffusion layer-type SGT structure (conventional SGT structure indicated by the point 2200) is provided at any value of the height Ld other than zero, which is proven that the SGT structure has a small off-leak current.

FIG. 24 shows a dependence of the punch-through voltage on the diameter Td which varies according to a change in shape of the concave drain diffusion layer. As seen in FIG. 24, in the concave drain diffusion layer-type SGT structure, a higher punch-through voltage as compared with the horizontally flat source/drain diffusion layer-type SGT structure (conventional SGT structure indicated by the point 2400) is also provided at any value of the diameter Td other than zero, which is proven that the SGT structure has a small off-leak current.

Based on a structure illustrated in FIG. 20, the following discussion will be made about the height Ls. In a complete depletion-type SGT, a depletion layer in the entire silicon pillar is divided into four depletion layers extending from respective ones of the gate, a source diffusion layer, and a base portion and a side portion of the concave drain diffusion layer. When an applied voltage is zero V, a depth of the depletion layer 2210 extending from the base portion of the concave drain diffusion layer is Td/4. Thus, as a prerequisite to suppressing a punch-through effect due to contact between the depletion layer 2210 extending from the base portion of the concave drain diffusion layer and the depletion layer 2250 extending from the source diffusion layer, it is essential that the height Ld is greater than the depth “Td/4” of the depletion layer. In other words, it is essential to satisfy the following relation (3-1):

$\begin{matrix} {{Ld} > \frac{Td}{4}} & \left( {3\text{-}1} \right) \end{matrix}$ Further, in a process for making the concave diffusion layer-type SGT structure illustrated in FIG. 16, it is necessary to perform ion implantation at an oblique angle as shown in FIG. 21 so as to form the concave diffusion layer. During the ion implantation, for example, when As⁺ is implanted into an NMOSFET, a silicon pillar of an NMOSFET adjacent to the target NMOSFET is likely to disturb the ion implantation. Thus, it is essential to satisfy the following relation (3-2):

$\begin{matrix} {{{\tan\left( \frac{\pi}{36} \right)} > \frac{{Ld} + {Lg} + {Ljs} + {Ljd}}{Tspace}},} & \left( {3\text{-}2} \right) \end{matrix}$

wherein: Ld is a height of the first-conductive type impurity region 610;

Lg is a length of the gate;

Ljd is a depth of the second-conductive type high-concentration impurity region 610; and

Ljs is a depth of the second-conductive type high-concentration impurity region 620; and

Tspace is a distance between silicon pillars of adjacent two SGTs.

Thus, based on the relation (3-2), Ld is required to satisfy the following relation (3-3):

$\begin{matrix} {{{{\tan\left( \frac{\pi}{36} \right)} \cdot {Tspace}} - \left( {{Lg} + {Ljs} + {Ljd}} \right)} > {Ld}} & \left( {3\text{-}3} \right) \end{matrix}$ (Fourth Embodiment) Semiconductor Device

FIG. 26 is a schematic bird's-eye view of a transistor as a semiconductor device of the present invention, wherein the third silicon pillar 830 in the first embodiment is formed as a high resistance region, instead of a first-conductive type impurity region, and each of the first-conductive type impurity region of the first silicon pillar 810 and the first-conductive type impurity region of the second silicon pillar 820 in the first embodiment is formed as a high resistance region. FIG. 27 is a schematic sectional view taken along the cutting-plane line a-a′ in FIG. 26, and FIG. 28 is a schematic sectional view taken along the cutting-plane line b-b′ in FIG. 27. FIG. 29 is a schematic sectional view taken along the cutting-plane line c-c′ in FIG. 27, and FIG. 30 is a schematic sectional view taken along the cutting-plane line d-d′ in FIG. 27. In the semiconductor device according to the fourth embodiment, in view of providing a higher punch-through voltage, it is desirable that each of a high resistance region 1010 provided in a first silicon pillar 810, and a high resistance region 1020 provided in a second silicon pillar 820, has a sufficiently-large area. In other words, it is desirable that a diameter Td and a height Ld of the high resistance region 1010, and a diameter Ts and a height Ls of the high resistance region 1020, are sufficiently large.

Specifically, assuming a structure in which: a length of a gate 210 is 100 nm; a film thickness of a gate dielectric is 2 nm; a diameter of the first silicon pillar 810 is 100 nm; and a height of each of the second silicon pillar 820 and a third silicon pillar 840 is 100 nm, a simulation was performed. As a simulation result on this structure, FIG. 41 shows a structure dependence of the punch-through voltage. The vertical axis of FIG. 41 represents the punch-through voltage Vpt which is a voltage applied to a drain electrode so as to cause a drain current of 1e-7A/um under a condition that a voltage applied to each of a gate electrode and a source electrode is zero V. The horizontal axis represents the heights Ls, Ld which vary according to a change in shape of respective ones of a concave source diffusion layer and a concave drain diffusion layer. As seen in FIG. 41, in the concave source/drain diffusion layer-type SGT structure (polygonal line 4101), a higher punch-through voltage as compared with the horizontally flat source/drain diffusion layer-type SGT structure (conventional SGT structure indicated by the point 4100) is provided at any value of each of the heights Ls, Ld other than zero, which is proven that the SGT structure has a small off-leak current. FIG. 17 shows a dependence of each of the heights Ls, Ld on the gate length Lg.

FIG. 42 shows a dependence of the punch-through voltage (vertical axis) on each of the diameters Ts, Td (horizontal axis) which vary according to a change in shape of respective ones of the concave source diffusion layer and the concave drain diffusion layer. As seen in FIG. 42, in the concave source/drain diffusion layer-type SGT structure (polygonal line 4201), a higher punch-through voltage as compared with the horizontally flat source/drain diffusion layer-type SGT structure (conventional SGT structure indicated by the point 4200) is also provided at any value of each of the diameters Ts, Td other than zero, which is proven that the SGT structure has a small off-leak current.

In the fourth embodiment, as with the first embodiment, it is desirable to satisfy the following relations (4-1) and (4-2) to provide a higher punch-through voltage:

$\begin{matrix} {{Ls} > \frac{Ts}{4}} & \left( {4\text{-}1} \right) \\ {{Ld} > \frac{Td}{4}} & \left( {4\text{-}2} \right) \end{matrix}$

Further, in the fourth embodiment, it is necessary to satisfy the following relation (4-3), as with the first embodiment, to prevent a silicon pillar of a MOSFET adjacent to a target MOSFET from disturbing ion implantation into the target MOSFET:

$\begin{matrix} {{{{\tan\left( \frac{\pi}{36} \right)} \cdot {Tspace}} - \left( {{Lg} + {Ljs} + {Ljd}} \right)} > {{Ls} + {Ld}}} & \left( {4\text{-}3} \right) \end{matrix}$ (Fifth Embodiment) Semiconductor Device

FIG. 31 is a schematic bird's-eye view of a transistor as a semiconductor device of the present invention, wherein the silicon pillar 830 in the second embodiment is formed as a high resistance region, instead of a first-conductive type impurity region, and the first-conductive type impurity region of the silicon pillar 820 in the second embodiment is formed as a high resistance region. FIG. 32 is a schematic sectional view taken along the cutting-plane line a-a′ in FIG. 31, and FIG. 33 is a schematic sectional view taken along the cutting-plane line b-b′ in FIG. 32. FIG. 34 is a schematic sectional view taken along the cutting-plane line c-c′ in FIG. 32, and FIG. 35 is a schematic sectional view taken along the cutting-plane line d-d′ in FIG. 32. In the fifth embodiment, in view of providing a higher punch-through voltage, it is desirable that a high resistance region 520 provided in a second silicon pillar 820 has a sufficiently-large area. In other words, it is desirable that a diameter Ts and a height Ls are sufficiently large.

Specifically, assuming a structure in which: a length of a gate 210 is 100 nm; a film thickness of a gate dielectric is 2 nm; a diameter of a first silicon pillar 810 is 100 nm; and a height of each of the second silicon pillar 820 and a third silicon pillar 840 is 100 nm, a simulation was performed. As a simulation result on this structure, FIG. 41 shows a structure dependence of the punch-through voltage. The vertical axis of FIG. 41 represents the punch-through voltage Vpt which is a voltage applied to a drain electrode so as to cause a drain current of 1e-7A/um under a condition that a voltage applied to each of a gate electrode and a source electrode is zero V. The horizontal axis represents the height Ls which varies according to a change in shape of a concave source diffusion layer. As seen in FIG. 41, in the concave source diffusion layer-type SGT structure (polygonal line 4102), a higher punch-through voltage as compared with the horizontally flat source/drain diffusion layer-type SGT structure (conventional SGT structure indicated by the point 4100) is provided at any value of the height Ls other than zero, which is proven that the SGT structure has a small off-leak current.

FIG. 42 shows a dependence of the punch-through voltage on the Ts and Td which varies according to a change in shape of the concave source diffusion layer. As seen in FIG. 42, in the concave source diffusion layer-type SGT structure (polygonal line 4202), a higher punch-through voltage as compared with the horizontally flat source/drain diffusion layer-type SGT structure (conventional SGT structure indicated by the point 4200) is also provided at any value of the diameter Ts other than zero, which is proven that the SGT structure has a small off-leak current.

In the fifth embodiment, as with the second embodiment, it is desirable to satisfy the following relation (5-1) to provide a higher punch-through voltage:

$\begin{matrix} {{Ls} > \frac{Ts}{4}} & \left( {5\text{-}1} \right) \end{matrix}$

Further, in the fifth embodiment, it is necessary to satisfy the following relation (5-2), as with the second embodiment, to prevent a silicon pillar of a MOSFET adjacent to a target MOSFET from disturbing ion implantation into the target MOSFET:

$\begin{matrix} {{{{\tan\left( \frac{\pi}{36} \right)} \cdot {Tspace}} - \left( {{Lg} + {Ljs} + {Ljd}} \right)} > {Ls}} & \left( {5\text{-}2} \right) \end{matrix}$ (Sixth Embodiment) Semiconductor Device

FIG. 36 is a schematic bird's-eye view of a transistor as a semiconductor device of the present invention, wherein the silicon pillar 830 in the third embodiment is formed as a high resistance region, instead of a first-conductive type impurity region, and the first-conductive type impurity region of the silicon pillar 810 in the third embodiment is formed as a high resistance region. FIG. 37 is a schematic sectional view taken along the cutting-plane line a-a′ in FIG. 36, and FIG. 38 is a schematic sectional view taken along the cutting-plane line b-b′ in FIG. 37. FIG. 39 is a schematic sectional view taken along the cutting-plane line c-c′ in FIG. 37, and FIG. 40 is a schematic sectional view taken along the cutting-plane line d-d′ in FIG. 37. The semiconductor device according to the sixth embodiment comprises a first-conductive type third silicon pillar 840, a first dielectric 310 surrounding a side surface of the third silicon pillar 840, a gate 210 surrounding the dielectric 310, a first silicon layer 810 provided underneath the third silicon pillar 840, and a second silicon pillar 820 provided on a top of the third silicon pillar 840, wherein: the first silicon pillar 810 has a second-conductive type high-concentration impurity region 610, and a high resistance region 1010 formed therein and surrounded by the second-conductive type high-concentration impurity region 610; and the second silicon pillar 820 is formed as a second-conductive type high-concentration impurity region 710.

In the sixth embodiment, in view of providing a higher punch-through voltage, it is desirable that the high resistance region 1010 of the first silicon pillar 810 has a sufficiently-large area. In other words, it is desirable that a diameter Td and a height Ld of the high resistance region 1010 are sufficiently large.

Specifically, assuming a structure in which: a length of the gate 210 is 100 nm; a film thickness of the gate dielectric is 2 nm; a diameter of the first silicon pillar 810 is 100 nm; and a height of each of the second silicon pillar 820 and the third silicon pillar 840 is 100 nm, a simulation was performed. As a simulation result on this structure, FIG. 41 shows a structure dependence of the punch-through voltage. The vertical axis of FIG. 41 represents the punch-through voltage Vpt which is a voltage applied to a drain electrode so as to cause a drain current of 1e-7A/um under a condition that a voltage applied to each of a gate electrode and a source electrode is zero V. The horizontal axis represents the height Ld which varies according to a change in shape of the concave drain diffusion layer. As seen in FIG. 41, in the concave drain diffusion layer-type SGT structure (polygonal line 4103), a higher punch-through voltage as compared with the horizontally flat source/drain diffusion layer-type SGT structure (conventional SGT structure indicated by the point 4100) is provided at any value of the height Ld other than zero, which is proven that the SGT structure has a small off-leak current.

FIG. 42 shows a dependence of the punch-through voltage on the diameter Td which varies according to a change in shape of the concave drain diffusion layer. As seen in FIG. 42, in the concave drain diffusion layer-type SGT structure (polygonal line 4203), a higher punch-through voltage as compared with the horizontally flat source/drain diffusion layer-type SGT structure (conventional SGT structure indicated by the point 4200) is also provided at any value of the diameter Td other than zero, which is proven that the SGT structure has a small off-leak current.

In the sixth embodiment, as with the third embodiment, it is desirable to satisfy the following relation (6-1) to provide a higher punch-through voltage,

$\begin{matrix} {{Ld} > \frac{Td}{4}} & \left( {6\text{-}1} \right) \end{matrix}$

Further, in the sixth embodiment, it is necessary to satisfy the following relation (6-2), as with the third embodiment, to prevent a silicon pillar of a MOSFET adjacent to a target MOSFET from disturbing ion implantation into the target MOSFET:

$\begin{matrix} {{{{\tan\left( \frac{\pi}{36} \right)} \cdot {Tspace}} - \left( {{Lg} + {Ljs} + {Ljd}} \right)} > {Ld}} & \left( {6\text{-}2} \right) \end{matrix}$ (Seventh Embodiment) Semiconductor Device

FIG. 43 is a bird's-eye view showing a transistor as a semiconductor device of the present invention. FIG. 44 is a schematic sectional view taken along the cutting-plane line a-a′ in FIG. 43, and FIG. 45 is a schematic sectional view taken along the cutting-plane line b-b′ in FIG. 44. FIG. 46 is a schematic sectional view taken along the cutting-plane line c-c′ in FIG. 44, and FIG. 47 is a schematic sectional view taken along the cutting-plane line d-d′ in FIG. 44. The semiconductor device according to the seventh embodiment comprises a first-conductive type first silicon pillar 830, a first dielectric 310 surrounding a side surface of the third silicon pillar 830, a gate 210 surrounding the dielectric 310, a first silicon pillar 810 provided underneath the third silicon pillar 830 to partially have a diameter greater than that of the third silicon pillar 830, and a second silicon pillar 820 provided on a top of the third silicon pillar 830 to partially have a diameter greater than that of the third silicon pillar 830, wherein: the first silicon pillar 810 has a second-conductive type high-concentration impurity region 610 formed in a surface thereof except at least a part of a contact surface region with the third silicon pillar 830, and a first-conductive type impurity region 510 formed therein and surrounded by the second-conductive type high-concentration impurity region 610; and the second silicon pillar 820 has a second-conductive type high-concentration impurity region 710 formed in a surface thereof except at least a part of a contact surface region with the third silicon pillar 830, and a first-conductive type impurity region 520 formed therein and surrounded by the second-conductive type high-concentration impurity region 710.

In the seventh embodiment, in view of providing a higher punch-through voltage, it is desirable that each of the first-conductive type impurity region 510 of the first silicon pillar 810 and the first-conductive type impurity region 520 of the second silicon pillar 820 has a sufficiently-large area. In other words, it is desirable that a diameter Td and a height Ld of the first-conductive type impurity region 510, and a diameter Ts and a height Ls of the first-conductive type impurity region 520, are sufficiently large.

Specifically, assuming a structure in which: a length of the gate 210 is 100 nm; a film thickness of the gate dielectric is 2 nm; a diameter of the first silicon pillar 810 is 100 nm; and a height of each of the second silicon pillar 820 and the third silicon pillar 830 is 100 nm, a simulation was performed. As a simulation result on this structure, FIG. 58 shows a dependence of the punch-through voltage on each of the diameters Ts, Td which vary according to a change in shape of respective ones of the concave source diffusion layer and the concave drain diffusion layer. As seen in FIG. 58, in the concave drain/source diffusion layer-type SGT structure (polygonal line 5801), a higher punch-through voltage as compared with the horizontally flat source/drain diffusion layer-type SGT structure (conventional SGT structure indicated by the point 5800) is provided at any value of each of the diameters Ts, Td other than zero, which is proven that the SGT structure has a small off-leak current.

In the seventh embodiment, as with the first embodiment, it is desirable to satisfy the following relations (7-1) and (7-2) to provide a higher punch-through voltage:

$\begin{matrix} {{Ls} > \frac{Ts}{4}} & \left( {7\text{-}1} \right) \\ {{Ld} > \frac{Td}{4}} & \left( {7\text{-}2} \right) \end{matrix}$

Further, in the seventh embodiment, it is necessary to satisfy the following relation (7-3), as with the first embodiment, to prevent a silicon pillar of a MOSFET adjacent to a target MOSFET from disturbing ion implantation into the target MOSFET:

$\begin{matrix} {{{{\tan\left( \frac{\pi}{36} \right)} \cdot {Tspace}} - \left( {{Lg} + {Ljs} + {Ljd}} \right)} > {{Ls} + {Ld}}} & \left( {7\text{-}3} \right) \end{matrix}$ (Eighth Embodiment) Semiconductor Device

FIG. 48 is a bird's-eye view showing a transistor as a semiconductor device of the present invention. FIG. 49 is a schematic sectional view taken along the cutting-plane line a-a′ in FIG. 48, and FIG. 50 is a schematic sectional view taken along the cutting-plane line b-b′ in FIG. 48. FIG. 51 is a schematic sectional view taken along the cutting-plane line c-c′ in FIG. 48, and FIG. 52 is a schematic sectional view taken along the cutting-plane line d-d′ in FIG. 48. The semiconductor device according to the eighth embodiment comprises a first-conductive type third silicon pillar 830, a first dielectric 310 surrounding a side surface of the third silicon pillar 830, a gate 210 surrounding the dielectric 310, a first silicon pillar 810 provided underneath the third silicon pillar 830 to partially have a diameter greater than that of the third silicon pillar 830, and a second silicon pillar 820 provided on a top of the third silicon pillar 830 to partially have a diameter greater than that of the third silicon pillar 830, wherein: the first silicon pillar 810 is formed as a second-conductive type high-concentration impurity region 610; and the second silicon pillar 820 has a second-conductive type high-concentration impurity region 710 formed in a surface thereof except at least a part of a contact surface region with the third silicon pillar 830, and a first-conductive type impurity region 520 formed therein and surrounded by the second-conductive type high-concentration impurity region 710.

In the eighth embodiment, in view of providing a higher punch-through voltage, it is desirable that the first-conductive type impurity region 520 of the second silicon pillar 820 has a sufficiently-large area. In other words, it is desirable that a diameter Ts and a height Ls of the first-conductive type impurity region 520 are sufficiently large.

Specifically, assuming a structure in which: a length of the gate 210 is 100 nm; a film thickness of the gate dielectric is 2 nm; a diameter of the first silicon pillar 810 is 100 nm; and a height of each of the second silicon pillar 820 and the third silicon pillar 830 is 100 nm, a simulation was performed. As a simulation result on this structure, FIG. 58 shows a dependence of the punch-through voltage on the Ts, Td which varies according to a change in shape of the concave source diffusion layer. As seen in FIG. 58, in the concave source diffusion layer-type SGT structure (polygonal line 5802), a higher punch-through voltage as compared with the horizontally flat source/drain diffusion layer-type SGT structure (conventional SGT structure indicated by the point 5800) is provided at any value of the Ts, Td other than zero, which is proven that the SGT structure has a small off-leak current.

In the eighth embodiment, as with the second embodiment, it is desirable to satisfy the following relation (8-1) to provide a higher punch-through voltage:

$\begin{matrix} {{Ls} > \frac{Ts}{4}} & \left( {8\text{-}1} \right) \end{matrix}$

Further, in the eighth embodiment, it is necessary to satisfy the following relation (8-2), as with the first embodiment, to prevent a silicon pillar of a MOSFET adjacent to a target MOSFET from disturbing ion implantation into the target MOSFET:

$\begin{matrix} {{{{\tan\left( \frac{\pi}{36} \right)} \cdot {Tspace}} - \left( {{Lg} + {Ljs} + {Ljd}} \right)} > {Ls}} & \left( {8\text{-}2} \right) \end{matrix}$ (Ninth Embodiment) Semiconductor Device

FIG. 53 is a bird's-eye view showing a transistor as a semiconductor device of the present invention. FIG. 54 is a schematic sectional view taken along the cutting-plane line a-a′ in FIG. 53, and FIG. 55 is a schematic sectional view taken along the cutting-plane line b-b′ in FIG. 54. FIG. 56 is a schematic sectional view taken along the cutting-plane line c-c′ in FIG. 54, and FIG. 57 is a schematic sectional view taken along the cutting-plane line d-d′ in FIG. 54. The semiconductor device according to the ninth embodiment comprises a first-conductive type third silicon pillar 830, a first dielectric 310 surrounding a side surface of the third silicon pillar 830, a gate 210 surrounding the dielectric 310, a first silicon pillar 810 provided underneath the third silicon pillar 830 to partially have a diameter greater than that of the third silicon pillar 830, and a second silicon pillar 820 provided on a top of the third silicon pillar 830 to partially have a diameter greater than that of the third silicon pillar 830, wherein: the first silicon pillar 810 has a second-conductive type high-concentration impurity region 610 formed in a surface thereof except at least a part of a contact surface region with the third silicon pillar 830, and a first-conductive type impurity region 510 formed therein and surrounded by the second-conductive type high-concentration impurity region 610; and the second silicon pillar 820 is formed as a second-conductive type high-concentration impurity region 710.

In the ninth embodiment, in view of providing a higher punch-through voltage, it is desirable that the first-conductive type impurity region 510 of the first silicon pillar 810 has a sufficiently-large area. In other words, it is desirable that a diameter Td and a height Ld of the first-conductive type impurity region 510 are sufficiently large.

Specifically, assuming a structure in which: a length of the gate 210 is 100 nm; a film thickness of the gate dielectric is 2 nm; a diameter of the first silicon pillar 810 is 100 nm; and a height of each of the second silicon pillar 820 and the third silicon pillar 830 is 100 nm, a simulation was performed. As a simulation result on this structure, FIG. 58 shows a dependence of the punch-through voltage on the Td which varies according to a change in shape of the concave drain diffusion layer. As seen in FIG. 58, in the concave drain diffusion layer-type SGT structure (polygonal line 5803), a higher punch-through voltage as compared with the horizontally flat source/drain diffusion layer-type SGT structure (conventional SGT structure indicated by the point 5800) is provided at any value of the diameter Td other than zero, which is proven that the SGT structure has a small off-leak current.

In the ninth embodiment, as with the third embodiment, it is desirable to satisfy the following relation (9-1) to provide a higher punch-through voltage:

$\begin{matrix} {{Ld} > \frac{Td}{4}} & \left( {9\text{-}1} \right) \end{matrix}$

Further, in the ninth embodiment, it is necessary to satisfy the following relation (9-2), as with the first embodiment, to prevent a silicon pillar of a MOSFET adjacent to a target MOSFET from disturbing ion implantation into the target MOSFET:

$\begin{matrix} {{{{\tan\left( \frac{\pi}{36} \right)} \cdot {Tspace}} - \left( {{Lg} + {Ljs} + {Ljd}} \right)} > {Ld}} & \left( {9\text{-}2} \right) \end{matrix}$ (Tenth Embodiment) Semiconductor Device

FIG. 59 is a schematic bird's-eye view of a transistor as a semiconductor device of the present invention, wherein the third silicon pillar 830 in the seventh embodiment is formed as a high resistance region, instead of a first-conductive type impurity region, and each of the first-conductive type impurity region of the first silicon pillar 810 and the first-conductive type impurity region of the second silicon pillar 820 in the seventh embodiment is formed as a high resistance region. FIG. 60 is a schematic sectional view taken along the cutting-plane line a-a′ in FIG. 59, and FIG. 61 is a schematic sectional view taken along the cutting-plane line b-b′ in FIG. 60. FIG. 62 is a schematic sectional view taken along the cutting-plane line c-c′ in FIG. 60, and FIG. 63 is a schematic sectional view taken along the cutting-plane line d-d′ in FIG. 60. In the semiconductor device according to the tenth embodiment, in view of providing a higher punch-through voltage, it is desirable that each of a high resistance region 1010 provided in a first silicon pillar 810, and a high resistance region 1020 provided in a second silicon pillar 820, has a sufficiently-large area. In other words, it is desirable that a diameter Td and a height Ld of the high resistance region 1010, and a diameter Ts and a height Ls of the high resistance region 1020, are sufficiently large.

Specifically, assuming a structure in which: a length of a gate 210 is 100 nm; a film thickness of a gate dielectric is 2 nm; a diameter of the first silicon pillar 810 is 100 nm; and a height of each of the second silicon pillar 820 and the third silicon pillar 830 is 100 nm, a simulation was performed. As a simulation result on this structure, FIG. 74 shows a dependence of the punch-through voltage on each of the diameters Ts, Td which vary according to a change in shape of respective ones of a concave source diffusion layer and a concave drain diffusion layer. As seen in FIG. 74, in the concave source/drain diffusion layer-type SGT structure (polygonal line 7401), a higher punch-through voltage as compared with the horizontally flat source/drain diffusion layer-type SGT structure (conventional SGT structure indicated by the point 7400) is also provided at any value of each of the diameters Ts, Td other than zero, which is proven that the SGT structure has a small off-leak current.

In the tenth embodiment, as with the first embodiment, it is desirable to satisfy the following relations (10-1) and (10-2) to provide a higher punch-through voltage:

$\begin{matrix} {{Ls} > \frac{Ts}{4}} & \left( {10\text{-}1} \right) \\ {{Ld} > \frac{Td}{4}} & \left( {10\text{-}2} \right) \end{matrix}$

Further, in the tenth embodiment, it is necessary to satisfy the following relation (10-3), as with the first embodiment, to prevent a silicon pillar of a MOSFET adjacent to a target MOSFET from disturbing ion implantation into the target MOSFET:

$\begin{matrix} {{{{\tan\left( \frac{\pi}{36} \right)} \cdot {Tspace}} - \left( {{Lg} + {Ljs} + {Ljd}} \right)} > {{Ls} + {Ld}}} & \left( {10\text{-}3} \right) \end{matrix}$ (Eleventh Embodiment) Semiconductor Device

FIG. 64 is a schematic bird's-eye view of a transistor as a semiconductor device of the present invention, wherein the third silicon pillar 830 in the eighth embodiment is formed as a high resistance region, instead of a first-conductive type impurity region, and the first-conductive type impurity region of the second silicon pillar 820 in the eighth embodiment is formed as a high resistance region. FIG. 65 is a schematic sectional view taken along the cutting-plane line a-a′ in FIG. 64, and FIG. 66 is a schematic sectional view taken along the cutting-plane line b-b′ in FIG. 65. FIG. 67 is a schematic sectional view taken along the cutting-plane line c-c′ in FIG. 65, and FIG. 68 is a schematic sectional view taken along the cutting-plane line d-d′ in FIG. 65. In the eleventh embodiment, in view of providing a higher punch-through voltage, it is desirable that a high resistance region 1020 provided in a second silicon pillar 820 has a sufficiently-large area. In other words, it is desirable that a diameter Ts and a height Ls are sufficiently large.

Specifically, assuming a structure in which: a length of a gate 210 is 100 nm; a film thickness of a gate dielectric is 2 nm; a diameter of a first silicon pillar 810 is 100 nm; and a height of each of the second silicon pillar 820 and a third silicon pillar 830 is 100 nm, a simulation was performed. As a simulation result on this structure, FIG. 74 shows a dependence of the punch-through voltage on the Ts, Td which varies according to a change in shape of a concave source diffusion layer. As seen in FIG. 74, in the concave source drain diffusion layer-type SGT structure (polygonal line 7402), a higher punch-through voltage as compared with the horizontally flat source/drain diffusion layer-type SGT structure (conventional SGT structure indicated by the point 7400) is also provided at any value of the Ts, Td other than zero, which is proven that the SGT structure has a small off-leak current.

In the eleventh embodiment, as with the second embodiment, it is desirable to satisfy the following relation (11-1) to provide a higher punch-through voltage:

$\begin{matrix} {{Ls} > \frac{Ts}{4}} & \left( {11\text{-}1} \right) \end{matrix}$

Further, in the eleventh embodiment, it is necessary to satisfy the following relation (11-2), as with the first embodiment, to prevent a silicon pillar of a MOSFET adjacent to a target MOSFET from disturbing ion implantation into the target MOSFET:

$\begin{matrix} {{{{\tan\left( \frac{\pi}{36} \right)} \cdot {Tspace}} - \left( {{Lg} + {Ljs} + {Ljd}} \right)} > {Ls}} & \left( {11\text{-}2} \right) \end{matrix}$ (Twelfth Embodiment) Semiconductor Device

FIG. 69 is a schematic bird's-eye view of a transistor as a semiconductor device of the present invention, wherein the silicon pillar 830 in the ninth embodiment is formed as a high resistance region, instead of a first-conductive type impurity region, and the first-conductive type impurity region of the silicon pillar 810 in the ninth embodiment is formed as a high resistance region. FIG. 70 is a schematic sectional view taken along the cutting-plane line a-a′ in FIG. 69, and FIG. 71 is a schematic sectional view taken along the cutting-plane line b-b′ in FIG. 70. FIG. 72 is a schematic sectional view taken along the cutting-plane line c-c′ in FIG. 70, and FIG. 73 is a schematic sectional view taken along the cutting-plane line d-d′ in FIG. 70.

In the twelfth embodiment, in view of providing a higher punch-through voltage, it is desirable that a high resistance region 1010 provided in a first silicon pillar 810 has a sufficiently-large area. In other words, it is desirable that a diameter Td and a height Ld of the high resistance region 1010 are sufficiently large.

Specifically, assuming a structure in which: a length of a gate 210 is 100 nm; a film thickness of a gate dielectric 310 is 2 nm; a diameter of the first silicon pillar 810 is 100 nm; and a height of each of a second silicon pillar 820 and a third silicon pillar 840 is 100 nm, a simulation was performed. As a simulation result on this structure, FIG. 74 shows a dependence of the punch-through voltage on the diameter Td which varies according to a change in shape of a concave drain diffusion layer. As seen in FIG. 74, in the concave source and drain diffusion layer-type SGT structures (polygonal line 7403), a higher punch-through voltage as compared with the horizontally flat source/drain diffusion layer-type SGT structure (conventional SGT structure indicated by the point 7400) is also provided at any value of the diameter Td other than zero, which is proven that the SGT structure has a small off-leak current.

In the twelfth embodiment, as with the third embodiment, it is desirable to satisfy the following relation (12-1) to provide a higher punch-through voltage,:

$\begin{matrix} {{Ld} > \frac{Td}{4}} & \left( {12\text{-}1} \right) \end{matrix}$

Further, in the twelfth embodiment, it is necessary to satisfy the following relation (12-2), as with the third embodiment, to prevent a silicon pillar of a MOSFET adjacent to a target MOSFET from disturbing ion implantation into the target MOSFET:

$\begin{matrix} {{{{\tan\left( \frac{\pi}{36} \right)} \cdot {Tspace}} - \left( {{Lg} + {Ljs} + {Ljd}} \right)} > {Ld}} & \left( {12\text{-}2} \right) \end{matrix}$ (Thirteenth Embodiment) Semiconductor Device

FIG. 75 is a schematic bird's-eye view of a transistor as a semiconductor device of the present invention. FIG. 76 is a schematic sectional view taken along the cutting-plane line a-a′ in FIG. 75. FIG. 77 is a schematic sectional view taken along the cutting-plane line b-b′ in FIG. 76, and FIG. 78 is a schematic sectional view taken along the cutting-plane line c-c′ in FIG. 76. The semiconductor device according to the thirteenth embodiment comprises a first-conductive type first silicon pillar 810 formed on a first-conductive type silicon substrate 100, a first dielectric 310 surrounding the first silicon pillar 810, a gate 210 surrounding the dielectric 310, and a second silicon pillar 820 provided on a top of the first silicon pillar 810, wherein: the silicon substrate 100 has a second-conductive type high-concentration impurity region 610 formed in a part thereof; and the second silicon layer 820 has a second-conductive type high-concentration impurity region 710 formed in a surface thereof except at least a part of a contact surface region with the third silicon pillar 810, and a first-conductive type impurity region 520 formed therein and surrounded by the second-conductive type high-concentration impurity region 710.

In the thirteenth embodiment, in view of providing a higher punch-through voltage, it is desirable that the first-conductive type impurity region 520 of the second silicon pillar 820 has a sufficiently-large area. In other words, it is desirable that a diameter Ts and a height Ls of the first-conductive type impurity region 520 are sufficiently large.

Specifically, assuming a structure in which: a length of the gate 210 is 100 nm; a film thickness of the gate dielectric is 2 nm; and a diameter of the first silicon pillar 810 is 100 nm; a height of the second silicon pillar 820 is 100 nm, a simulation was performed. As a simulation result on this structure, FIG. 79 shows a structure dependence of the punch-through voltage. The vertical axis of FIG. 79 represents the punch-through voltage Vpt which is a voltage applied to a drain electrode so as to cause a drain current of 1e-7A/um under a condition that a voltage applied to each of a gate electrode and a source electrode is zero V. The horizontal axis represents the height Ls which varies according to a change in shape of the concave source diffusion layer. As seen in FIG. 79, in the concave source diffusion layer-type SGT structure (polygonal line 7901), a higher punch-through voltage as compared with the horizontally flat source/drain diffusion layer-type SGT structure (conventional SGT structure indicated by the point 7900) is provided at any value of the height Ld other than zero, which is proven that the SGT structure has a small off-leak current.

FIG. 80 shows a dependence of the punch-through voltage on the diameters Ts which varies according to a change in shape of the concave source diffusion layer. As seen in FIG. 80, in the concave source diffusion layer-type SGT structure (polygonal line 8001), a higher punch-through voltage as compared with the horizontally flat source/drain diffusion layer-type SGT structure (conventional SGT structure indicated by the point 8000) is provided at any value of the diameter Ts other than zero, which is proven that the SGT structure has a small off-leak current.

In the thirteenth embodiment, it is desirable that the height Ls is greater than a depth Ts/4 of a depletion layer to suppress the punch-through effect, as with the first embodiment. In other words, it is desirable to satisfy the following relation (13-1):

$\begin{matrix} {{Ls} > \frac{Ts}{4}} & \left( {13\text{-}1} \right) \end{matrix}$

Further, in a process for making the concave diffusion layer-type SGT structure illustrated in FIG. 75, it is necessary to perform ion implantation at an oblique angle as shown in FIG. 81 so as to form the concave diffusion layer. During the ion implantation, for example, when As⁺ is implanted into an NMOSFET, a silicon pillar of an NMOSFET adjacent to the target NMOSFET is likely to disturb the ion implantation. Thus, it is essential to satisfy the following relation (13-2):

$\begin{matrix} {{{\tan\left( \frac{\pi}{36} \right)} > \frac{{Ls} + {Ljs}}{Tspace}},} & \left( {13\text{-}2} \right) \end{matrix}$

wherein: Ls is a height of the first-conductive type impurity region 610;

Ljs is a depth of the second-conductive type high-concentration impurity region 620; and

Tspace is a distance between silicon pillars of adjacent two SGTs; Thus, based on the relation (13-2), Ls is required to satisfy the following relation (12-3):

$\begin{matrix} {{{{\tan\left( \frac{\pi}{36} \right)} \cdot {Tspace}} - {Ljs}} > {Ls}} & \left( {13\text{-}3} \right) \end{matrix}$ (Fourteenth Embodiment) Semiconductor Device

FIG. 82 is a schematic bird's-eye view of a transistor as a semiconductor device of the present invention, wherein the third silicon pillar 830 in the embodiment is formed as a high resistance region, instead of a first-conductive type impurity region, and the first-conductive type impurity region of the second silicon pillar 820 in the embodiment is formed as a high resistance region. FIG. 83 is a schematic sectional view taken along the cutting-plane line a-a′ in FIG. 82. FIG. 84 is a schematic sectional view taken along the cutting-plane line b-b′ in FIG. 82, and FIG. 85 is a schematic sectional view taken along the cutting-plane line c-c′ in FIG. 82.

In the fourteenth embodiment, in view of providing a higher punch-through voltage, it is desirable that a high resistance region 1020 provided in a second silicon pillar 820 has a sufficiently-large area. In other words, it is desirable that a diameter Ts and a height Ls of the high resistance region 1020 are sufficiently large.

Specifically, assuming a structure in which: a length of a gate 210 is 100 nm; a film thickness of a gate dielectric is 2 nm; a diameter of a first silicon pillar 810 is 100 nm; and a height of the second silicon pillar 820 is 100 nm, a simulation was performed. As a simulation result on this structure, FIG. 86 shows a structure dependence of the punch-through voltage. The vertical axis of FIG. 86 represents the punch-through voltage Vpt which is a voltage applied to a drain electrode so as to cause a drain current of 1e-7A/um under a condition that a voltage applied to each of a gate electrode and a source electrode is zero V. The horizontal axis represents the height Ls which varies according to a change in shape of a concave source diffusion layer. As seen in FIG. 86, in the concave source diffusion layer-type SGT structure (polygonal line 8601), a higher punch-through voltage as compared with the horizontally flat source/drain diffusion layer-type SGT structure (conventional SGT structure indicated by the point 8600) is provided at any value of the height Ld other than zero, which is proven that the SGT structure has a small off-leak current.

FIG. 87 shows a dependence of the punch-through voltage on the diameter Ts which varies according to a change in shape of the concave source diffusion layer. As seen in FIG. 87, in the concave source diffusion layer-type SGT structure (polygonal line 8701), a higher punch-through voltage as compared with the horizontally flat source/drain diffusion layer-type SGT structure (conventional SGT structure indicated by the point 8700) is also provided at any value of the diameter Ts other than zero, which is proven that the SGT structure has a small off-leak current.

In the fourteenth embodiment, as with the thirteenth embodiment, it is desirable to satisfy the following relation (14-1) to provide a higher punch-through voltage:

$\begin{matrix} {{Ls} > \frac{Ts}{4}} & \left( {14\text{-}1} \right) \end{matrix}$

Further, in the fourteenth embodiment, it is necessary to satisfy the following relation (14-2), as with the third embodiment, to prevent a silicon pillar of a MOSFET adjacent to a target MOSFET from disturbing ion implantation into the target MOSFET:

$\begin{matrix} {{{{\tan\left( \frac{\pi}{36} \right)} \cdot {Tspace}} - {Ljs}} > {Ls}} & \left( {14\text{-}2} \right) \end{matrix}$ (Fifteenth Embodiment) Semiconductor Device

FIG. 88 is a schematic bird's-eye view of a transistor as a semiconductor device of the present invention. FIG. 89 is a schematic sectional view taken along the cutting-plane line a-a′ in FIG. 88. FIG. 90 is a schematic sectional view taken along the cutting-plane line b-b′ in FIG. 89, and FIG. 91 is a schematic sectional view taken along the cutting-plane line c-c′ in FIG. 89. The semiconductor device according to the fifteenth embodiment comprises a first-conductive type fourth silicon pillar 840 formed on a first-conductive type silicon substrate 100, a first dielectric 310 surrounding the fourth silicon pillar 810, a gate 210 surrounding the dielectric 310, and a first silicon pillar 810 provided on a top of the fourth silicon pillar 840, wherein: the silicon substrate 100 has a second-conductive type high-concentration impurity region 710 formed in a part thereof; and the first silicon layer 810 has a second-conductive type high-concentration impurity region 610 formed in a surface thereof except at least a part of a contact surface region with the fourth silicon pillar, and a first-conductive type impurity region 520 formed therein and surrounded by the second-conductive type high-concentration impurity region 610.

In the fifteenth embodiment, in view of providing a higher punch-through voltage, it is desirable that the first-conductive type impurity region 510 of the first silicon pillar 810 has a sufficiently-large area. In other words, it is desirable that a diameter Ts and a height Td of the first-conductive type impurity region 510 are sufficiently large.

Specifically, assuming a structure in which: a length of the gate 210 is 100 nm; a film thickness of the gate dielectric is 2 nm; and a diameter of the fourth silicon pillar 840 is 100 nm; a height of the first silicon pillar 810 is 100 nm, a simulation was performed. As a simulation result on this structure, FIG. 92 shows a structure dependence of the punch-through voltage. The vertical axis of FIG. 92 represents the punch-through voltage Vpt which is a voltage applied to a drain electrode so as to cause a drain current of 1e-7A/um under a condition that a voltage applied to each of a gate electrode and a source electrode is zero V. The horizontal axis represents the height Ls which varies according to a change in shape of the concave source diffusion layer. As seen in FIG. 92, in the concave source and drain diffusion layer-type SGT structures (polygonal line 9201), a higher punch-through voltage as compared with the horizontally flat source/drain diffusion layer-type SGT structure (conventional SGT structure indicated by the point 9200) is provided at any value of the height Ld other than zero, which is proven that the SGT structure has a small off-leak current.

FIG. 93 shows a dependence of the punch-through voltage on the diameters Ts which varies according to a change in shape of the concave source diffusion layer. As seen in FIG. 93, in the concave source and drain diffusion layer-type SGT structures (polygonal line 9301), a higher punch-through voltage as compared with the horizontally flat source/drain diffusion layer-type SGT structure (conventional SGT structure indicated by the point 9300) is provided at any value of the diameter Ts other than zero, which is proven that the SGT structure has a small off-leak current.

In the fifteenth embodiment, it is desirable that the height Ls is greater than a depth Ts/4 of a depletion layer to suppress the punch-through effect, as with the first embodiment. In other words, it is desirable to satisfy the following relation (15-1):

$\begin{matrix} {{Ld} > \frac{Td}{4}} & \left( {15\text{-}1} \right) \end{matrix}$

Further, in a process for making the concave diffusion layer-type SGT structure illustrated in FIG. 88, it is necessary to perform ion implantation at an oblique angle as shown in FIG. 94 so as to form the concave diffusion layer. During the ion implantation, for example, when As⁺ is implanted into an NMOSFET, a silicon pillar of an NMOSFET adjacent to the target NMOSFET is likely to disturb the ion implantation. Thus, it is essential to satisfy the following relation (15-2):

$\begin{matrix} {{{\tan\left( \frac{\pi}{36} \right)} > \frac{{Ld} + {Ljd}}{Tspace}},} & \left( {15\text{-}2} \right) \end{matrix}$

wherein: Ld is a height of the first-conductive type impurity region 510;

Ljd is a depth of the second-conductive type high-concentration impurity region 610; and

Tspace is a distance between silicon pillars of adjacent two SGTs;

Thus, based on the relation (15-2), Ls is required to satisfy the following relation (15-3):

$\begin{matrix} {{{{\tan\left( \frac{\pi}{36} \right)} \cdot {Tspace}} - {Ljd}} > {Ld}} & \left( {15\text{-}3} \right) \end{matrix}$ (Sixteenth Embodiment) Semiconductor Device

FIG. 95 is a schematic bird's-eye view of a transistor as a semiconductor device of the present invention, wherein the third silicon pillar 830 in the embodiment is formed as a high resistance region, instead of a first-conductive type impurity region, and the first-conductive type impurity region of the second silicon pillar 820 in the embodiment is formed as a high resistance region. FIG. 96 is a schematic sectional view taken along the cutting-plane line a-a′ in FIG. 95. FIG. 97 is a schematic sectional view taken along the cutting-plane line b-b′ in FIG. 96, and FIG. 98 is a schematic sectional view taken along the cutting-plane line c-c′ in FIG. 96.

In the sixteenth embodiment, in view of providing a higher punch-through voltage, it is desirable that a high resistance region 1010 provided in a first silicon pillar 810 has a sufficiently-large area. In other words, it is desirable that a diameter Ts and a height Ls of the high resistance region 1010 are sufficiently large.

Specifically, assuming a structure in which: a length of a gate 210 is 100 nm; a film thickness of a gate dielectric is 2 nm; a diameter of a fourth silicon pillar 840 is 100 nm; and a height of the first silicon pillar 810 is 100 nm, a simulation was performed. As a simulation result on this structure, FIG. 99 shows a structure dependence of the punch-through voltage. The vertical axis of FIG. 99 represents the punch-through voltage Vpt which is a voltage applied to a drain electrode so as to cause a drain current of 1e-7A/um under a condition that a voltage applied to each of a gate electrode and a source electrode is zero V. The horizontal axis represents the height Ld which varies according to a change in shape of a concave source diffusion layer. As seen in FIG. 99, in the concave source diffusion layer-type SGT structure (polygonal line 9901), a higher punch-through voltage as compared with the horizontally flat source/drain diffusion layer-type SGT structure (conventional SGT structure indicated by the point 9900) is provided at any value of the height Ld other than zero, which is proven that the SGT structure has a small off-leak current.

FIG. 100 shows a dependence of the punch-through voltage on the diameter Td which varies according to a change in shape of the concave drain diffusion layer. As seen in FIG. 100, in the concave drain diffusion layer-type SGT structure (polygonal line 10001), a higher punch-through voltage as compared with the horizontally flat source/drain diffusion layer-type SGT structure (conventional SGT structure indicated by the point 10000) is also provided at any value of the diameter Ts other than zero, which is proven that the SGT structure has a small off-leak current.

In the sixteenth embodiment, as with the fifteenth embodiment, it is desirable to satisfy the following relation (16-1) to provide a higher punch-through voltage:

$\begin{matrix} {{Ld} > \frac{Td}{4}} & \left( {16\text{-}1} \right) \end{matrix}$

Further, in the sixteenth embodiment, it is necessary to satisfy the following relation (16-2), as with the third embodiment, to prevent a silicon pillar of a MOSFET adjacent to a target MOSFET from disturbing ion implantation into the target MOSFET:

$\begin{matrix} {{{{\tan\left( \frac{\pi}{36} \right)} \cdot {Tspace}} - {Ljd}} > {Ld}} & \left( {16\text{-}2} \right) \end{matrix}$ (Seventeenth Embodiment) Semiconductor Device

FIG. 101 is a schematic bird's-eye view of a transistor as a semiconductor device of the present invention, wherein the first-conductive type impurity region of the first silicon layer 810 in the first embodiment is formed as a second-conductive type impurity region 511 including a region having an impurity concentration of 1E18 (cm⁻³) or less, and the first-conductive type impurity region of the second silicon layer 820 in the first embodiment is formed as a second-conductive type impurity region 521 including a region having an impurity concentration of 1E18 (cm⁻³) or less. FIG. 102 is a schematic sectional view taken along the cutting-plane line a-a′ in FIG. 101, and FIG. 103 is a schematic sectional view taken along the cutting-plane line b-b′ in FIG. 102. FIG. 104 is a schematic sectional view taken along the cutting-plane line c-c′ in FIG. 102, and FIG. 105 is a schematic sectional view taken along the cutting-plane line d-d′ in FIG. 102.

In the seventeenth embodiment, in view of providing a higher punch-through voltage, it is desirable that each of the second-conductive type low-concentration impurity region 511 of the first silicon pillar 810 including a region with an impurity concentration of 1E18 (cm⁻³) or less, and the second-conductive type low-concentration impurity region 521 of the second silicon pillar 820 including a region with an impurity concentration of 1E18 (cm⁻³) or less, has a sufficiently-large area. In other words, it is desirable that a diameter Td and a height Ld of the second-conductive type impurity region 511, and a diameter Ts and a height Ls of the second-conductive type impurity region 521, are sufficiently large.

In the seventeenth embodiment, as with the first embodiment, it is desirable to satisfy the following relations (17-1) and (17-2) to provide a higher punch-through voltage:

$\begin{matrix} {{Ls} > \frac{Ts}{4}} & \left( {17\text{-}1} \right) \\ {{Ld} > \frac{Td}{4}} & \left( {17\text{-}2} \right) \end{matrix}$

Further, in the seventeenth embodiment, it is necessary to satisfy the following relation (17-3), as with the first embodiment, to prevent a silicon pillar of a MOSFET adjacent to a target MOSFET from disturbing ion implantation into the target MOSFET:

$\begin{matrix} {{{{\tan\left( \frac{\pi}{36} \right)} \cdot {Tspace}} - \left( {{Lg} + {Ljs} + {Ljd}} \right)} > {{Ls} + {Ld}}} & \left( {17\text{-}3} \right) \end{matrix}$ (Eighteenth Embodiment) Semiconductor Device

FIG. 106 is a schematic bird's-eye view of a transistor as a semiconductor device of the present invention, wherein the first-conductive type impurity region of the second silicon layer 820 in the second embodiment is formed as a second-conductive type impurity region 521 including a region having an impurity concentration of 1E18 (cm⁻³) or less. FIG. 107 is a schematic sectional view taken along the cutting-plane line a-a′ in FIG. 106, and FIG. 108 is a schematic sectional view taken along the cutting-plane line b-b′ in FIG. 107. FIG. 109 is a schematic sectional view taken along the cutting-plane line c-c′ in FIG. 107, and FIG. 110 is a schematic sectional view taken along the cutting-plane line d-d′ in FIG. 107.

In the eighteenth embodiment, in view of providing a higher punch-through voltage, it is desirable that the second-conductive type low-concentration impurity region 521 of the second silicon pillar 820 including a region with an impurity concentration of 1E18 (cm⁻³) or less has a sufficiently-large area. In other words, it is desirable that a diameter Ts and a height Ls are sufficiently large.

In the eighteenth embodiment, as with the second embodiment, it is desirable to satisfy the following relation (18-1) to provide a higher punch-through voltage:

$\begin{matrix} {{Ls} > \frac{Ts}{4}} & \left( {18\text{-}1} \right) \end{matrix}$

Further, in the eighteenth embodiment, it is necessary to satisfy the following relation (18-2), as with the second embodiment, to prevent a silicon pillar of a MOSFET adjacent to a target MOSFET from disturbing ion implantation into the target MOSFET:

$\begin{matrix} {{{{\tan\left( \frac{\pi}{36} \right)} \cdot {Tspace}} - \left( {{Lg} + {Ljs} + {Ljd}} \right)} > {Ls}} & \left( {18\text{-}2} \right) \end{matrix}$ (Nineteenth Embodiment) Semiconductor Device

FIG. 111 is a schematic bird's-eye view of a transistor as a semiconductor device of the present invention, wherein the first-conductive type impurity region of the silicon layer 810 in the third embodiment is formed as a second-conductive type impurity region 511 including a region having an impurity concentration of 1E18 (cm⁻³) or less. FIG. 112 is a schematic sectional view taken along the cutting-plane line a-a′ in FIG. 111, and FIG. 113 is a schematic sectional view taken along the cutting-plane line b-b′ in FIG. 112. FIG. 114 is a schematic sectional view taken along the cutting-plane line c-c′ in FIG. 112, and FIG. 114 is a schematic sectional view taken along the cutting-plane line d-d′ in FIG. 112.

The semiconductor device according to the nineteenth embodiment comprises a first-conductive type third silicon pillar 830, a first dielectric 310 surrounding a side surface of the third silicon pillar 830, a gate 210 surrounding the dielectric 310, a first silicon layer 810 provided underneath the third silicon pillar 830, and a second silicon pillar 820 provided on a top of the third silicon pillar 830, wherein: the first silicon pillar 810 has a second-conductive type high-concentration impurity region 610, and a second-conductive type low-concentration impurity region 511 formed therein to have an impurity concentration of 1E18 (cm⁻³) or less and surrounded by the second-conductive type high-concentration impurity region 610; and the second silicon pillar 820 is formed as a second-conductive type high-concentration impurity region 710.

In the nineteenth embodiment, in view of providing a higher punch-through voltage, it is desirable that the first-conductive type impurity region 511 of the first silicon pillar 810 has a sufficiently-large area. In other words, it is desirable that a diameter Ts and a height Ls are sufficiently large.

$\begin{matrix} {{Ld} > \frac{Td}{4}} & \left( {19\text{-}1} \right) \end{matrix}$

Further, in the nineteenth embodiment, it is necessary to satisfy the following relation (19-2), as with the third embodiment, to prevent a silicon pillar of a MOSFET adjacent to a target MOSFET from disturbing ion implantation into the target MOSFET:

$\begin{matrix} {{{{\tan\left( \frac{\pi}{36} \right)} \cdot {Tspace}} - \left( {{Lg} + {Ljs} + {Ljd}} \right)} > {Ld}} & \left( {19\text{-}2} \right) \end{matrix}$ (Twentieth Embodiment) Semiconductor Device

FIG. 116 is a schematic bird's-eye view of a transistor as a semiconductor device of the present invention, wherein the first-conductive type impurity region of the first silicon layer 810 in the seventh embodiment is formed as a second-conductive type impurity region 511 including a region having an impurity concentration of 1E18 (cm⁻³) or less, and the first-conductive type impurity region of the silicon layer 820 in the seventh embodiment is formed as a second-conductive type impurity region 521. FIG. 117 is a schematic sectional view taken along the cutting-plane line a-a′ in FIG. 116, and FIG. 118 is a schematic sectional view taken along the cutting-plane line b-b′ in FIG. 117. FIG. 118 is a schematic sectional view taken along the cutting-plane line c-c′ in FIG. 117, and FIG. 119 is a schematic sectional view taken along the cutting-plane line d-d′ in FIG. 117.

In the semiconductor device according to the twentieth embodiment, in view of providing a higher punch-through voltage, it is desirable that each of the second-conductive type low-concentration impurity region 511 of the first silicon pillar 810 including a region with an impurity concentration of 1E18 (cm⁻³) or less, and the second-conductive type low-concentration impurity region 521 of the second silicon pillar 820 including a region with an impurity concentration of 1E18 (cm³) or less, has a sufficiently-large area. In other words, it is desirable that a diameter Td and a height Ld of the second-conductive type impurity region 511, and a diameter Ts and a height Ls of the second-conductive type impurity region 521, are sufficiently large.

In the twentieth embodiment, as with the first embodiment, it is desirable to satisfy the following relations (20-1) and (20-2) to provide a higher punch-through voltage:

$\begin{matrix} {{Ls} > \frac{Ts}{4}} & \left( {20\text{-}1} \right) \\ {{Ld} > \frac{Td}{4}} & \left( {20\text{-}2} \right) \end{matrix}$

Further, in the twentieth embodiment, it is necessary to satisfy the following relation (20-3), as with the first embodiment, to prevent a silicon pillar of a MOSFET adjacent to a target MOSFET from disturbing ion implantation into the target MOSFET:

$\begin{matrix} {{{{\tan\left( \frac{\pi}{36} \right)} \cdot {Tspace}} - \left( {{Lg} + {Ljs} + {Ljd}} \right)} > {{Ls} + {Ld}}} & \left( {20\text{-}3} \right) \end{matrix}$ (Twenty-First Embodiment) Semiconductor Device

FIG. 121 is a schematic bird's-eye view of a transistor as a semiconductor device of the present invention, wherein the first-conductive type impurity region of the silicon layer 820 in the eighth embodiment is formed as a second-conductive type impurity region 521 including a region having an impurity concentration of 1E18 (cm⁻³) or less. FIG. 122 is a schematic sectional view taken along the cutting-plane line a-a′ in FIG. 121, and FIG. 123 is a schematic sectional view taken along the cutting-plane line b-b′ in FIG. 122. FIG. 124 is a schematic sectional view taken along the cutting-plane line c-c′ in FIG. 122, and FIG. 124 is a schematic sectional view taken along the cutting-plane line d-d′ in FIG. 122.

In the twenty-first embodiment, in view of providing a higher punch-through voltage, it is desirable that the second-conductive type low-concentration impurity region 2320 of the second silicon pillar 820 has a sufficiently-large area. In other words, it is desirable that a diameter Ts and a height Ls are sufficiently large.

In the twenty-first embodiment, in view of providing a higher punch-through voltage, it is desirable that the second-conductive type low-concentration impurity region 521 of the second silicon pillar 820 including a region with an impurity concentration of 1E18 (cm⁻³) or less has a sufficiently-large area. In other words, it is desirable that a diameter Ts and a height Ls of the second-conductive type impurity region 521 are sufficiently large.

In the twenty-first embodiment, as with the second embodiment, it is desirable to satisfy the following relation (21-1) to provide a higher punch-through voltage:

$\begin{matrix} {{Ls} > \frac{Ts}{4}} & \left( {21\text{-}1} \right) \end{matrix}$

Further, in the twenty-first embodiment, it is necessary to satisfy the following relation (21-2), as with the first embodiment, to prevent a silicon pillar of a MOSFET adjacent to a target MOSFET from disturbing ion implantation into the target MOSFET:

$\begin{matrix} {{{{\tan\left( \frac{\pi}{36} \right)} \cdot {Tspace}} - \left( {{Lg} + {Ljs} + {Ljd}} \right)} > {Ls}} & \left( {21\text{-}2} \right) \end{matrix}$ (Twenty-Second Embodiment) Semiconductor Device

FIG. 126 is a schematic bird's-eye view of a transistor as a semiconductor device of the present invention, wherein the first-conductive type impurity region of the silicon layer 810 in the ninth embodiment is formed as a second-conductive type impurity region 511 including a region having an impurity concentration of 1E18 (cm⁻³) or less. FIG. 127 is a schematic sectional view taken along the cutting-plane line a-a′ in FIG. 126, and FIG. 128 is a schematic sectional view taken along the cutting-plane line b-b′ in FIG. 127. FIG. 129 is a schematic sectional view taken along the cutting-plane line c-c′ in FIG. 127, and FIG. 130 is a schematic sectional view taken along the cutting-plane line d-d′ in FIG. 127.

In the twenty-second embodiment, in view of providing a higher punch-through voltage, it is desirable that the second-conductive type low-concentration impurity region 511 of the first silicon pillar 810 including a region with an impurity concentration of 1E18 (cm⁻³) or less has a sufficiently-large area. In other words, it is desirable that a diameter Ts and a height Ls of the second-conductive type impurity region 511 are sufficiently large.

In the twenty-second embodiment, as with the third embodiment, it is desirable to satisfy the following relation (22-1) to provide a higher punch-through voltage:

$\begin{matrix} {{Ld} > \frac{Td}{4}} & \left( {22\text{-}1} \right) \end{matrix}$

Further, in the twenty-second embodiment, it is necessary to satisfy the following relation (22-2), as with the third embodiment, to prevent a silicon pillar of a MOSFET adjacent to a target MOSFET from disturbing ion implantation into the target MOSFET:

$\begin{matrix} {{{{\tan\left( \frac{\pi}{36} \right)} \cdot {Tspace}} - \left( {{Lg} + {Ljs} + {Ljd}} \right)} > {Ld}} & \left( {22\text{-}2} \right) \end{matrix}$ (Twenty-Third Embodiment) Semiconductor Device

FIG. 131 is a schematic bird's-eye view of a transistor as a semiconductor device of the present invention, wherein the first-conductive type impurity region of the second silicon layer 820 in the fifteenth embodiment is formed as a second-conductive type impurity region 521 including a region having an impurity concentration of 1E18 (cm⁻³) or less. FIG. 132 is a schematic sectional view taken along the cutting-plane line a-a′ in FIG. 131. FIG. 133 is a schematic sectional view taken along the cutting-plane line b-b′ in FIG. 132, and FIG. 134 is a schematic sectional view taken along the cutting-plane line c-c′ in FIG. 132.

In the twenty-third embodiment, in view of providing a higher punch-through voltage, it is desirable that the second-conductive type low-concentration impurity region 521 of the second silicon pillar 820 including a region with an impurity concentration of 1E18 (cm⁻³) or less has a sufficiently-large area. In other words, it is desirable that a diameter Ts and a height Ls of the second-conductive type impurity region 521 are sufficiently large.

In the twenty-third embodiment, as with the fifteenth embodiment, it is desirable to satisfy the following relation (23-1) to provide a higher punch-through voltage:

$\begin{matrix} {{Ls} > \frac{Ts}{4}} & \left( {23\text{-}1} \right) \end{matrix}$

Further, in the twenty-third embodiment, it is necessary to satisfy the following relation (23-2), as with the fifteenth embodiment, to prevent a silicon pillar of a MOSFET adjacent to a target MOSFET from disturbing ion implantation into the target MOSFET:

$\begin{matrix} {{{{\tan\left( \frac{\pi}{36} \right)} \cdot {Tspace}} - \left( {{Lg} + {Ljs} + {Ljd}} \right)} > {Ls}} & \left( {23\text{-}2} \right) \end{matrix}$ (Twenty-Fourth Embodiment) Semiconductor Device

FIG. 135 is a schematic bird's-eye view of a transistor as a semiconductor device of the present invention, wherein the first-conductive type impurity region of the first silicon layer 810 in the sixteenth embodiment is formed as a second-conductive type impurity region 511 including a region having an impurity concentration of 1E18 (cm⁻³) or less. FIG. 136 is a schematic sectional view taken along the cutting-plane line a-a′ in FIG. 135. FIG. 137 is a schematic sectional view taken along the cutting-plane line b-b′ in FIG. 136, and FIG. 138 is a schematic sectional view taken along the cutting-plane line c-c′ in FIG. 136.

In the twenty-fourth embodiment, in view of providing a higher punch-through voltage, it is desirable that the second-conductive type low-concentration impurity region 511 of the first silicon pillar 810 including a region with an impurity concentration of 1E18 (cm⁻³) or less has a sufficiently-large area. In other words, it is desirable that a diameter Ts and a height Ls of the second-conductive type impurity region 511 are sufficiently large.

In the twenty-fourth embodiment, as with the sixteenth embodiment, it is desirable to satisfy the following relation (24-1) to provide a higher punch-through voltage:

$\begin{matrix} {{Ld} > \frac{Td}{4}} & \left( {24\text{-}1} \right) \end{matrix}$

Further, in the twenty-fourth embodiment, it is necessary to satisfy the following relation (24-2), as with the sixteenth embodiment, to prevent a silicon pillar of a MOSFET adjacent to a target MOSFET from disturbing ion implantation into the target MOSFET:

$\begin{matrix} {{{{\tan\left( \frac{\pi}{36} \right)} \cdot {Tspace}} - \left( {{Lg} + {Ljs} + {Ljd}} \right)} > {Ld}} & \left( {24\text{-}2} \right) \end{matrix}$

EXPLANATORY OF CODES

-   -   100, 110: semiconductor substrate     -   210: gate     -   310: gate dielectric film     -   410: first high-concentration impurity region     -   411: second high-concentration impurity region     -   510, 520: first high-concentration impurity region with a         concentration of 1.9E18 (cm⁻³) or less     -   511, 521: second high-concentration impurity region with a         concentration of 1.9E18 (cm⁻³) or less     -   610: drain     -   710: source     -   810, 820, 830, 840: silicon pillar     -   910: element isolation dielectric film     -   1010, 1020, 1030: high resistance region     -   1110: oxide film-based sidewall     -   1210: contact hole-etching stopper layer     -   1310: source     -   1410: drain     -   1610: channel region     -   1710: metal interconnection portion     -   1810: Al     -   1910: concave semiconductor     -   2010: second high-concentration impurity region     -   2110: second low-concentration impurity region     -   2210: depletion layer extending from base portion of concave         drain     -   2220: depletion layer extending from side portion of concave         drain     -   2230: depletion layer extending from base portion of concave         source     -   2240: depletion layer extending from side portion of concave         source     -   2250: depletion layer extending from drain     -   2260: depletion layer extending from source     -   2270: depletion layer extending from gate 

What is claimed is:
 1. A semiconductor device comprising: a first-conductive type first silicon pillar on a first-conductive type silicon substrate: a first dielectric surrounding a side surface of the first silicon pillar; a gate surrounding the dielectric; and a third silicon pillar on a top of the first silicon pillar, wherein: the silicon substrate has a second-conductive type high-concentration impurity region formed in a part thereof; and the third silicon pillar including a second-conductive type high-concentration impurity region in a peripheral surface thereof except in at least a central portion of a contact surface region with the first silicon pillar, the central portion characterized by a diameter that is less than a diameter of the third silicon pillar, and a first-conductive type impurity region therein and surrounded by the second-conductive type high-concentration impurity, where the second-conductive type is of an opposite conductivity to the first conductive type and thereby a p-n junction resides at an interface thereof, and wherein the first-conductive type impurity region has a length that extends from a base portion of the second-conductive type high-concentration impurity region to the contact surface region, and the length is greater than that of a depletion layer extending from the base portion.
 2. The semiconductor device as defined in claim 1, which satisfies the following relation: ${{Ls} > \frac{Ts}{4}},$ wherein Ls and Ts are, respectively, a length and a diameter of the first-conductive type impurity region of the third silicon pillar on a source side.
 3. The semiconductor device as defined in claim 1, which satisfies the following relation: ${{Ld} > \frac{Td}{4}},$ wherein Ld and Td are, respectively, a length and a diameter of the first-conductive type impurity region of the third silicon pillar on a drain side.
 4. The semiconductor device as defined in claim 1, wherein: the first silicon pillar is comprises a high resistance region; the second-conductive type impurity region of the silicon substrate is comprises a high resistance region; and the first-conductive type impurity region of the third silicon pillar comprises a high resistance region.
 5. A semiconductor device comprising: a first-conductive type first silicon pillar on a first-conductive type silicon substrate: a first dielectric surrounding a side surface of the first silicon pillar; a gate surrounding the dielectric; and a third silicon pillar on a top of the first silicon pillar, wherein: the silicon substrate includes a second-conductive type high-concentration impurity region in a part thereof; and the third silicon pillar includes a second-conductive type high-concentration impurity region in a peripheral surface thereof except in at least a part of a contact surface region with the first silicon pillar, the central portion characterized by a diameter that is less than a diameter of the third silicon pillar, and a first-conductive type impurity region therein and surrounded by the second-conductive type high-concentration impurity region, where the second-conductive type is of an opposite conductivity to the first conductive type and thereby a p-n junction resides at an interface thereof, and wherein the first-conductive type impurity region has a length that extends from a base portion of the second-conductive type high-concentration impurity region to the contact surface region, which is short enough to allow the second-conductive type high-concentration impurity region of the third silicon pillar to be formed.
 6. The semiconductor device as defined in claim 5, wherein: the first silicon pillar comprise a high resistance region; the second-conductive type impurity region of the silicon substrate comprises a high resistance region; and the first-conductive type impurity region of the third silicon pillar comprises a high resistance region.
 7. A semiconductor device comprising: a first-conductive type first silicon pillar formed on a first-conductive type silicon substrate: a first dielectric surrounding a side surface of the first silicon pillar; a gate surrounding the dielectric; and a third silicon pillar provided on a top of the first silicon pillar, wherein: the silicon substrate has a second-conductive type high-concentration impurity region formed in a part thereof; and the third silicon pillar has a second-conductive type high-concentration impurity region formed in a surface thereof except at least a part of a contact surface region with the first silicon pillar, and a first-conductive type impurity region formed therein and surrounded by the second-conductive type high-concentration impurity region of the third silicon pillar, and wherein the first-conductive type impurity region of the third silicon pillar has a length which is short enough to allow the second-conductive type high-concentration impurity region of the third silicon pillar to be formed and which satisfies the following relation: ${{{{\tan\left( \frac{\pi}{36} \right)} \cdot {Tspace}} - {Ljs}} > {Ls}},$ wherein: Tspace is a distance between adjacent two of a plurality of the semiconductor devices formed on the silicon substrate; Ljs is a depth of the second-conductive type high-concentration impurity region formed in the third silicon pillar to serve as a source; and Ls is a length of the first-conductive type impurity region of the third silicon pillar.
 8. A semiconductor device comprising: a first-conductive type first silicon pillar formed on a first-conductive type silicon substrate: a first dielectric surrounding a side surface of the first silicon pillar; a gate surrounding the dielectric; and a third silicon pillar provided on a top of the first silicon pillar, wherein: the silicon substrate has a second-conductive type high-concentration impurity region formed in a part thereof; and the third silicon pillar has a second-conductive type high-concentration impurity region formed in a surface thereof except at least a part of a contact surface region with the first silicon pillar, and a first-conductive type impurity region formed therein and surrounded by the second-conductive type high-concentration impurity region of the third silicon pillar, and wherein the first-conductive type impurity region of the third silicon pillar has a length which is short enough to allow the second-conductive type high-concentration impurity region of the third silicon pillar to be formed and which satisfies the following relation: ${{{{\tan\left( \frac{\pi}{36} \right)} \cdot {Tspace}} - {Ljd}} > {Ld}},$ wherein: Tspace is a distance between adjacent two of a plurality of the semiconductor devices formed on the silicon substrate; Ljd is a depth of the second-conductive type high-concentration impurity region formed in the third silicon pillar to serve as a drain; and Ld is a length of the first-conductive type impurity region of the third silicon pillar. 